Sunday, January 30, 2011

Hot off the presses! Jan 01 UNKNOWN

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Latest Articles Include:

  • Chemistry on a global stage
    - UNKNOWN 6(1):1 (2011)
    Nature Nanotechnology | Editorial Chemistry on a global stage Journal name:Nature NanotechnologyVolume: 6,Page:1Year published:(2011)DOI:doi:10.1038/nnano.2011.276Published online23 December 2010 Read the full article * FREE access with registration Register now * Already have a Nature.com account? Login Additional access options: * Use a document delivery service * Login via Athens * Purchase a site license * Institutional access * British Library Document Supply Centre * Infotrieve * Thompson ISI Document Delivery * You can also request this document from your local library through inter-library loan services. The International Year of Chemistry gives chemists a chance to raise the profile of their subject. View full text Read the full article * FREE access with registration Register now * Already have a Nature.com account? Login Additional access options: * Use a document delivery service * Login via Athens * Purchase a site license * Institutional access * British Library Document Supply Centre * Infotrieve * Thompson ISI Document Delivery * You can also request this document from your local library through inter-library loan services. Additional data
  • Science in the service of citizens and consumers
    - UNKNOWN 6(1):3-4 (2011)
    Nature Nanotechnology | Thesis Science in the service of citizens and consumers * Chris Toumey1 Contact Chris Toumey Search for this author in: * NPG journals * PubMed * Google ScholarJournal name:Nature NanotechnologyVolume: 6,Pages:3–4Year published:(2011)DOI:doi:10.1038/nnano.2011.263Published online23 December 2010 Read the full article * Instant access to this article: US$32Buy now * Subscribe to Nature Nanotechnology for full access: SubscribeLogin for existing subscribers Additional access options: * Use a document delivery service * Login via Athens * Purchase a site license * Institutional access * British Library Document Supply Centre * Infotrieve * Thompson ISI Document Delivery * You can also request this document from your local library through inter-library loan services. A new approach to public knowledge of science focuses on what the public want to know rather than what scientists think they should know. Chris Toumey reports. View full text Subject terms: * Ethical, legal and other societal issues Author information Article tools * Full text * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg Affiliations * Chris Toumey is at the University of South Carolina NanoCenter. Toumey@mailbox.sc.edu Read the full article * Instant access to this article: US$32Buy now * Subscribe to Nature Nanotechnology for full access: SubscribeLogin for existing subscribers Additional access options: * Use a document delivery service * Login via Athens * Purchase a site license * Institutional access * British Library Document Supply Centre * Infotrieve * Thompson ISI Document Delivery * You can also request this document from your local library through inter-library loan services. Additional data
  • Our choice from the recent literature
    - UNKNOWN 6(1):5 (2011)
    Nature Nanotechnology | Research Highlights Our choice from the recent literature Journal name:Nature NanotechnologyVolume: 6,Page:5Year published:(2011)DOI:doi:10.1038/nnano.2011.269Published online23 December 2010 Read the full article * Instant access to this article: US$32Buy now * Subscribe to Nature Nanotechnology for full access: SubscribeLogin for existing subscribers Additional access options: * Use a document delivery service * Login via Athens * Purchase a site license * Institutional access * British Library Document Supply Centre * Infotrieve * Thompson ISI Document Delivery * You can also request this document from your local library through inter-library loan services. © 2010 ACS Nano Lett. doi:10.1021/nl1033304 (2010) View full text Read the full article * Instant access to this article: US$32Buy now * Subscribe to Nature Nanotechnology for full access: SubscribeLogin for existing subscribers Additional access options: * Use a document delivery service * Login via Athens * Purchase a site license * Institutional access * British Library Document Supply Centre * Infotrieve * Thompson ISI Document Delivery * You can also request this document from your local library through inter-library loan services. Additional data
  • Scanning tunnelling microscopy: Closing in on molecular junctions
    - UNKNOWN 6(1):7-8 (2011)
    Nature Nanotechnology | News and Views Scanning tunnelling microscopy: Closing in on molecular junctions * Andreas Heinrich1 Contact Andreas Heinrich Search for this author in: * NPG journals * PubMed * Google ScholarJournal name:Nature NanotechnologyVolume: 6,Pages:7–8Year published:(2011)DOI:doi:10.1038/nnano.2011.266Published online23 December 2010 Read the full article * Instant access to this article: US$18Buy now * Subscribe to Nature Nanotechnology for full access: SubscribeLogin for existing subscribers Additional access options: * Use a document delivery service * Login via Athens * Purchase a site license * Institutional access * British Library Document Supply Centre * Infotrieve * Thompson ISI Document Delivery * You can also request this document from your local library through inter-library loan services. Contacts between a single molecule and a metal electrode can be good or bad depending on the number of metal atoms that are in direct contact with the molecule. View full text Subject terms: * Electronic properties and devices * Surface patterning and imaging Author information Article tools * Full text * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg Affiliations * Andreas Heinrich is in the IBM Research Division, Almaden Research Center, San Jose, California 95120, USA. heinrich@almaden.ibm.com Read the full article * Instant access to this article: US$18Buy now * Subscribe to Nature Nanotechnology for full access: SubscribeLogin for existing subscribers Additional access options: * Use a document delivery service * Login via Athens * Purchase a site license * Institutional access * British Library Document Supply Centre * Infotrieve * Thompson ISI Document Delivery * You can also request this document from your local library through inter-library loan services. Additional data
  • Nanoelectronics: Graphene gets a better gap
    - UNKNOWN 6(1):8-9 (2011)
    Nature Nanotechnology | News and Views Nanoelectronics: Graphene gets a better gap * Stephan Roche1 Contact Stephan Roche Search for this author in: * NPG journals * PubMed * Google ScholarJournal name:Nature NanotechnologyVolume: 6,Pages:8–9Year published:(2011)DOI:doi:10.1038/nnano.2011.262Published online23 December 2010 Read the full article * Instant access to this article: US$18Buy now * Subscribe to Nature Nanotechnology for full access: SubscribeLogin for existing subscribers Additional access options: * Use a document delivery service * Login via Athens * Purchase a site license * Institutional access * British Library Document Supply Centre * Infotrieve * Thompson ISI Document Delivery * You can also request this document from your local library through inter-library loan services. Graphene nanoribbons with low defect densities and large energy gaps can be fabricated by chemically unzipping carbon nanotubes and annealing the result. View full text Subject terms: * Electronic properties and devices * Synthesis and processing Author information Article tools * Full text * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg Affiliations * Stephan Roche is at the Catalan Institute of Nanotechnology (ICN-ICREA) and CIN2, Campus UAB, 08193, Bellaterra, Barcelona, Spain. stephan.roche@icn.cat Read the full article * Instant access to this article: US$18Buy now * Subscribe to Nature Nanotechnology for full access: SubscribeLogin for existing subscribers Additional access options: * Use a document delivery service * Login via Athens * Purchase a site license * Institutional access * British Library Document Supply Centre * Infotrieve * Thompson ISI Document Delivery * You can also request this document from your local library through inter-library loan services. Additional data
  • Quantum computing: Solid-state spins survive
    - UNKNOWN 6(1):9-11 (2011)
    Nature Nanotechnology | News and Views Quantum computing: Solid-state spins survive * Michael J. Biercuk1 Contact Michael J. Biercuk Search for this author in: * NPG journals * PubMed * Google Scholar * David J. Reilly1 Contact David J. Reilly Search for this author in: * NPG journals * PubMed * Google Scholar * AffiliationsJournal name:Nature NanotechnologyVolume: 6,Pages:9–11Year published:(2011)DOI:doi:10.1038/nnano.2011.261Published online23 December 2010 Read the full article * Instant access to this article: US$18Buy now * Subscribe to Nature Nanotechnology for full access: SubscribeLogin for existing subscribers Additional access options: * Use a document delivery service * Login via Athens * Purchase a site license * Institutional access * British Library Document Supply Centre * Infotrieve * Thompson ISI Document Delivery * You can also request this document from your local library through inter-library loan services. Quantum-control pulse sequences can suppress errors and significantly extend the lifetimes of spin-based quantum bits in solid-state devices. View full text Subject terms: * Nanomagnetism and spintronics * Quantum information Author information Article tools * Full text * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg Affiliations * Michael J. Biercuk and David J. Reilly are in the School of Physics, University of Sydney, New South Wales 2006, Australia. michael.biercuk@sydney.edu.au; david.reilly@sydney.edu.au Read the full article * Instant access to this article: US$18Buy now * Subscribe to Nature Nanotechnology for full access: SubscribeLogin for existing subscribers Additional access options: * Use a document delivery service * Login via Athens * Purchase a site license * Institutional access * British Library Document Supply Centre * Infotrieve * Thompson ISI Document Delivery * You can also request this document from your local library through inter-library loan services. Additional data
  • Nanobiotechnology: Nanoparticle coronas take shape
    - UNKNOWN 6(1):11-12 (2011)
    Nature Nanotechnology | News and Views Nanobiotechnology: Nanoparticle coronas take shape * Marco P. Monopoli1 Contact Marco P. Monopoli Search for this author in: * NPG journals * PubMed * Google Scholar * Francesca Baldelli Bombelli1 Contact Francesca Baldelli Bombelli Search for this author in: * NPG journals * PubMed * Google Scholar * Kenneth A. Dawson1 Contact Kenneth A. Dawson Search for this author in: * NPG journals * PubMed * Google Scholar * AffiliationsJournal name:Nature NanotechnologyVolume: 6,Pages:11–12Year published:(2011)DOI:doi:10.1038/nnano.2011.267Published online23 December 2010 Read the full article * Instant access to this article: US$18Buy now * Subscribe to Nature Nanotechnology for full access: SubscribeLogin for existing subscribers Additional access options: * Use a document delivery service * Login via Athens * Purchase a site license * Institutional access * British Library Document Supply Centre * Infotrieve * Thompson ISI Document Delivery * You can also request this document from your local library through inter-library loan services. Understanding the impact of nanomaterials on human health will require more detailed knowledge about the protein corona that surrounds nanoparticles in biological environments. View full text Subject terms: * Nanomedicine * Nanoparticles Author information Article tools * Full text * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg Affiliations * Marco P. Monopoli, Francesca Baldelli Bombelli and Kenneth A. Dawson are in the Centre for BioNano Interactions, University College Dublin, Belfield, Dublin 4, Ireland. marco.monopoli@cbni.ucd.ie; francesca.baldelli@cbni.ucd.ie; kenneth.a.dawson@cbni.ucd.ie Read the full article * Instant access to this article: US$18Buy now * Subscribe to Nature Nanotechnology for full access: SubscribeLogin for existing subscribers Additional access options: * Use a document delivery service * Login via Athens * Purchase a site license * Institutional access * British Library Document Supply Centre * Infotrieve * Thompson ISI Document Delivery * You can also request this document from your local library through inter-library loan services. Additional data
  • Nanotechnological strategies for engineering complex tissues
    - UNKNOWN 6(1):13-22 (2011)
    Nature Nanotechnology | Review Nanotechnological strategies for engineering complex tissues * Tal Dvir1, 2 Search for this author in: * NPG journals * PubMed * Google Scholar * Brian P. Timko2, 3 Search for this author in: * NPG journals * PubMed * Google Scholar * Daniel S. Kohane2 Search for this author in: * NPG journals * PubMed * Google Scholar * Robert Langer1 Contact Robert Langer Search for this author in: * NPG journals * PubMed * Google Scholar * Affiliations * Corresponding authorJournal name:Nature NanotechnologyVolume: 6,Pages:13–22Year published:(2011)DOI:doi:10.1038/nnano.2010.246Published online12 December 2010 Abstract * Abstract * Author information Article tools * Full text * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg Tissue engineering aims at developing functional substitutes for damaged tissues and organs. Before transplantation, cells are generally seeded on biomaterial scaffolds that recapitulate the extracellular matrix and provide cells with information that is important for tissue development. Here we review the nanocomposite nature of the extracellular matrix, describe the design considerations for different tissues and discuss the impact of nanostructures on the properties of scaffolds and their uses in monitoring the behaviour of engineered tissues. We also examine the different nanodevices used to trigger certain processes for tissue development, and offer our view on the principal challenges and prospects of applying nanotechnology in tissue engineering. View full text Subject terms: * Nanobiotechnology * Nanomaterials * Nanomedicine Figures at a glance * Figure 1: An example of a tissue engineering concept that involves seeding cells within porous biomaterial scaffolds. , Cells are isolated from the patient and may be cultivated () in vitro on two-dimensional surfaces for efficient expansion. , Next, the cells are seeded in porous scaffolds together with growth factors, small molecules, and micro- and/or nanoparticles. The scaffolds serve as a mechanical support and a shape-determining material, and their porous nature provides high mass transfer and waste removal. , The cell constructs are further cultivated in bioreactors to provide optimal conditions for organization into a functioning tissue. , Once a functioning tissue has been successfully engineered, the construct is transplanted on the defect to restore function. * Figure 2: The information provided to cells by the extracellular matrix (ECM). , ECM fibres provide cells with topographical features that trigger morphogenesis. Adhesion proteins such as fibronectin and laminin located on the fibres interact with the cells through their transmembrane integrin receptors to initiate intracellular signalling cascades, which affect most aspects of cell behaviour. Polysaccharides such as hyaluronic acid and heparan sulphate act as a compression buffer against the stress, or serve as a growth factor depot. , Illustrations of the heart, liver and bone at the level of organ (left) and tissue and cell/matrix interaction (centre), followed by scanning electron micrographs of engineered scaffolds (right). The ECMs of various tissues have different composition and spatial organization of molecules to maintain specific tissue morphologies. For example (), the ECM of muscle tissues, such as the heart, forces the heart cells (cardiomyocytes) to couple mechanically to each other and to form elongated and aligned cell bundles that cre! ate an anisotropic syncytium. Nanogrooved surfaces (SEM image) are suitable matrices for cardiac tissue engineering because they force cardiomyocytes to align. , Cells composing epithelial tissues are polarized and contact three types of surfaces for efficient mass transfer: the ECM, other cells and a lumen. Nanofibres modified with surface molecules can promote cell adhesion and tissue polarity (SEM images). , Bone is a nanocomposite material consisting primarily of a collagen-rich organic matrix and inorganic hydroxyapatite nanocrystallites, which serve as a chelating agent for mineralization of osteoblasts. The scaffold structure (SEM image), stiffness and hydroxyapatite nanopatterning on the surface (inset) can enhance osteoblast spreading and bone tissue formation. SEM images reproduced with permission from: , ref. 56, © 2010 NAS; , ref. 59, © 2009 Elsevier; , ref. 65, © 2010 Elsevier. * Figure 3: Recreating ECM components using nanoscale tools. , ECM nanofibres produced by electrospinning polymeric fibres contain nanoparticles that release epidermal growth factor (green) and bovine serum albumin (red) in parallel. , Self-assembled peptide amphiphile nanofibres. , Alginate scaffolds containing short motifs of ECM adhesion proteins such as RGD encouraged mesenchymal stem cells to spread and attach to the matrix (), whereas on unmodified scaffolds () only cell–cell interactions were seen (collagen fibres, green; nuclei, red). , Epithelial cells respond to nanopatterning by alignment and elongation along the grating axis. , On smooth substrates, cells are mostly rounded. Figures reproduced with permission from: , ref. 28, © 2009 Wiley; , ref. 32, © 2009 AAAS; and , ref. 42, © 2009 Elsevier; and , ref. 48, © 2003 Company of Biologists. * Figure 4: Nanodevices in tissue engineering. , Three-dimensional, free-standing nanowire transistor probe for electrical recording. The probe is composed of a kinked nanowire (yellow arrow) and a flexible substrate material. The device is used to penetrate the membrane of living cells (inset) and measure intracellular signals (lower panel). , Biosensors based on carbon nanotubes are used for the detection of genotoxic analytes, including chemotherapeutic drugs and reactive oxygen species. Upper figure shows a schematic of a sensor made from a DNA and a single-walled carbon nanotube complex bound to a glass surface through a biotin-BSA (orange) and neutravidin (blue) linkage. Lower figures reveal the spectral changes arising from the interaction of the nanotube sensor with (from left to right): a chemotherapeutic agent, hydrogen peroxide, singlet oxygen and hydroxyl radicals (blue curve, before addition of analytes; green curve, after addition of analytes). Figures reproduced with permission from: , ref. 99, © 2010 AAA! S; , 101 © 2010 NPG. Author information * Abstract * Author information Affiliations * Department of Chemical Engineering, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA * Tal Dvir & * Robert Langer * Laboratory for Biomaterials and Drug Delivery, Department of Anesthesiology, Division of Critical Care Medicine, Children's Hospital Boston, Harvard Medical School, 300 Longwood Avenue, Boston, Massachusetts 02115, USA * Tal Dvir, * Brian P. Timko & * Daniel S. Kohane * Harvard-Massachusetts Institute of Technology Division of Health Sciences and Technology, Cambridge, Massachusetts 02139, USA. * Brian P. Timko Competing financial interests R.L. has a financial interest in Pervasis and Fibrocell Science, Inc. Corresponding author Correspondence to: * Robert Langer Additional data
  • Atomic-scale engineering of electrodes for single-molecule contacts
    - UNKNOWN 6(1):23-27 (2011)
    Nature Nanotechnology | Letter Atomic-scale engineering of electrodes for single-molecule contacts * Guillaume Schull1 Contact Guillaume Schull Search for this author in: * NPG journals * PubMed * Google Scholar * Thomas Frederiksen2 Contact Thomas Frederiksen Search for this author in: * NPG journals * PubMed * Google Scholar * Andrés Arnau2, 3, 4 Search for this author in: * NPG journals * PubMed * Google Scholar * Daniel Sánchez-Portal2, 3 Search for this author in: * NPG journals * PubMed * Google Scholar * Richard Berndt5 Search for this author in: * NPG journals * PubMed * Google Scholar * Affiliations * Contributions * Corresponding authorsJournal name:Nature NanotechnologyVolume: 6,Pages:23–27Year published:(2011)DOI:doi:10.1038/nnano.2010.215Received02 September 2010Accepted07 October 2010Published online14 November 2010 Abstract * Abstract * Author information * Supplementary information Article tools * Full text * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg The transport of charge through a conducting material depends on the intrinsic ability of the material to conduct current and on the charge injection efficiency at the contacts between the conductor and the electrodes carrying current to and from the material1, 2, 3. According to theoretical considerations4, this concept remains valid down to the limit of single-molecule junctions5. Exploring this limit in experiments requires atomic-scale control of the junction geometry. Here we present a method for probing the current through a single C60 molecule while changing, one by one, the number of atoms in the electrode that are in contact with the molecule. We show quantitatively that the contact geometry has a strong influence on the conductance. We also find a crossover from a regime in which the conductance is limited by charge injection at the contact to a regime in which the conductance is limited by scattering at the molecule. Thus, the concepts of 'good' and 'bad' ! contacts, commonly used in macro- and mesoscopic physics, can also be applied at the molecular scale. View full text Subject terms: * Electronic properties and devices * Surface patterning and imaging Figures at a glance * Figure 1: STM images of atomically engineered electrodes on Cu(111). , Constant-current STM image of CuN clusters on a Cu(111) surface obtained with a copper-terminated STM tip (I = 0.1 nA; sample voltage Vs = 0.1 V). , Image obtained with a C60-terminated STM tip (I = 0.1 nA; Vs = −1.7 V). The CuN clusters work as tips for 'reverse imaging' of the C60 fixed at the tip apex17. The threefold symmetric patterns reveal that one of the hexagons of the C60 cage is facing the surface. Standing waves related to surface states are not visible at this sample voltage. Both images, 18.2 nm × 7.2 nm. * Figure 2: Transport measurements of a single C60 molecule in contact with an increasing number of atoms. , Conductance in units of G0 (on a logarithmic scale) versus distance for a C60 tip approaching a bare Cu(111) surface (black line) and a surface covered with CuN clusters (coloured lines). One of the hexagons of the C60 cage is facing the surface. The distance scale was established from the apparent height of each cluster in STM images recorded at I = 100 pA and Vs = −0.1 V. Hereafter, with the same settings, the STM feedback was opened for collecting conductance data. Crosses mark the experimental contact points defined as the intersection of the contact and transition regimes (dashed grey lines indicate the bare surface data). Insets: geometry (bottom left) and list (right) of the experimental conductances at contact (Gc) derived from the conductance traces. zc is the contact distance. , STM image (I = 100 pA; Vs = 0.1 V; 8.0 × 2.3 nm2) of Cu2 and linear Cu3 recorded with a copper tip. –, STM images (I = 100 pA; Vs = −0.1 V; 8.0 × 2.3 nm2) of the same area recorde! d with a C60 tip. After the image in was recorded, the approach of the C60 tip caused the Cu2 cluster to move ~1.3 nm to the right (), after which the approach of the tip to the linear Cu3 cluster caused it to adopt a more compact configuration (). ,, Simulation showing how a linear Cu3 (, red circles) relaxes into a triangular configuration () as the distance between a C60 tip and the surface is reduced from 18 Å to 17.2 Å. The orange circles represent the Cu(111) surface; the carbon atoms are shown in grey. * Figure 3: Conductances at contact between a single C60 molecule and clusters of copper atoms. , Normalized conductance at contact versus cluster size N. Experimental data from six different molecular tips are shown, as well as theoretical data for two electrode separations around the point of contact (L1 = 17.2 Å and L2 = 18.0 Å, measured between the second-topmost layers). Conductance is normalized to the value for a single C60 molecule in contact with a 16-atom cluster. , Normalized conductance at contact per atom in the cluster versus cluster size N. ,, Calculated PDOS onto the atomic basis orbitals (s, p and d character) of CuN () and C60 () versus energy for seven different cluster sizes and for a separation of L1 = 17.2 Å. Inset to : the PDOS of CuN at the Fermi energy varies linearly with N. * Figure 4: Scattering at the contact between a single C60 molecule and clusters of copper atoms. Visualization of the scattering states at the Fermi energy for different numbers of contacting atoms. The calculated isosurfaces (shown in grey) represent the electron density in the junction at the centre of the Brillouin zone for a sum over the first three (most transmitting) eigenchannels (electron waves coming from below)20. Data were calculated for clusters with N = 1, … , 7 and 16 adatoms at an electrode separation L1 = 17.2 Å (measured between the second-topmost layers). Not all copper atoms in the cluster are visible. The scattering states are only calculated in the region of space defined by the topmost copper surface layers. Author information * Abstract * Author information * Supplementary information Affiliations * Institut de Physique et Chimie des Matériaux de Strasbourg, UMR 7504 (CNRS – Université de Strasbourg), 67034 Strasbourg, France * Guillaume Schull * Donostia International Physics Center (DIPC), 20018 San Sebastián, Spain * Thomas Frederiksen, * Andrés Arnau & * Daniel Sánchez-Portal * Centro de Fisica de Materiales CSIC-UPV/EHU, Materials Physics Center MPC, 20080 San Sebastián, Spain * Andrés Arnau & * Daniel Sánchez-Portal * Depto. Fisica de Materiales UPV/EHU, Facultad de Quimica, 20080 San Sebastián, Spain * Andrés Arnau * Institut für Experimentelle und Angewandte Physik, Christian-Albrechts-Universität zu Kiel, 24098 Kiel, Germany * Richard Berndt Contributions G.S. and R.B. provided the experimental concept. G.S. performed the STM and contact experiments. T.F. performed the first-principles calculations, and analysis was carried out with A.A. and D.S.P. All authors contibuted to the discussion of the results and preparation of the manuscript. Competing financial interests The authors declare no competing financial interests. Corresponding authors Correspondence to: * Guillaume Schull or * Thomas Frederiksen Supplementary information * Abstract * Author information * Supplementary information PDF files * Supplementary information (890 KB) Supplementary information Additional data
  • Freestanding palladium nanosheets with plasmonic and catalytic properties
    - UNKNOWN 6(1):28-32 (2011)
    Nature Nanotechnology | Letter Freestanding palladium nanosheets with plasmonic and catalytic properties * Xiaoqing Huang1 Search for this author in: * NPG journals * PubMed * Google Scholar * Shaoheng Tang1 Search for this author in: * NPG journals * PubMed * Google Scholar * Xiaoliang Mu1 Search for this author in: * NPG journals * PubMed * Google Scholar * Yan Dai1 Search for this author in: * NPG journals * PubMed * Google Scholar * Guangxu Chen1 Search for this author in: * NPG journals * PubMed * Google Scholar * Zhiyou Zhou1 Search for this author in: * NPG journals * PubMed * Google Scholar * Fangxiong Ruan2 Search for this author in: * NPG journals * PubMed * Google Scholar * Zhilin Yang2 Search for this author in: * NPG journals * PubMed * Google Scholar * Nanfeng Zheng1 Contact Nanfeng Zheng Search for this author in: * NPG journals * PubMed * Google Scholar * Affiliations * Contributions * Corresponding authorJournal name:Nature NanotechnologyVolume: 6,Pages:28–32Year published:(2011)DOI:doi:10.1038/nnano.2010.235Received14 July 2010Accepted29 October 2010Published online05 December 2010 Abstract * Abstract * Author information * Supplementary information Article tools * Full text * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg Ultrathin metal films can exhibit quantum size and surface effects that give rise to unique physical and chemical properties1, 2, 3, 4, 5, 6, 7. Metal films containing just a few layers of atoms can be fabricated on substrates using deposition techniques7, but the production of freestanding ultrathin structures remains a significant challenge. Here we report the facile synthesis of freestanding hexagonal palladium nanosheets that are less than 10 atomic layers thick, using carbon monoxide as a surface confining agent. The as-prepared nanosheets are blue in colour and exhibit a well-defined but tunable surface plasmon resonance peak in the near-infrared region. The combination of photothermal stability and biocompatibility makes palladium nanosheets promising candidates for photothermal therapy. The nanosheets also exhibit electrocatalytic activity for the oxidation of formic acid that is 2.5 times greater than that of commercial palladium black catalyst. View full text Subject terms: * Nanomaterials * Structural properties Figures at a glance * Figure 1: Characterization of ultrathin palladium nanosheets synthesized in the presence of PVP and CTAB in DMF. , TEM image of the palladium nanosheets. Inset: photograph of an ethanol dispersion of the as-prepared palladium nanosheets in a curvette. , HRTEM image of a palladium nanosheet flat lying on the TEM grid. , SAED pattern of a single palladium nanosheet (shown in the inset). , TEM image of the assembly of palladium nanosheets perpendicular to the TEM grid. Inset: thickness distribution of the palladium nanosheets. * Figure 2: TEM images of the palladium nanosheets produced under different reaction conditions. ,, Palladium nanosheets, collected following 0.5 h () and 1.5 h () reactions, using CTAB as the Br− source. ,, Nanosheets collected following 3 h reactions using NaBr () and TBAB () as the Br− source. , Larger nanosheets, grown using the palladium nanosheets in as seed particles. , Edge lengths of samples –. Error bars in are the standard deviations of the edge length distributions. * Figure 3: Optical absorption and photothermal properties of palladium nanosheets. , Absorption spectra of hexagonal palladium nanosheets with average edge lengths of 21, 27, 41 and 51 nm. , Photothermal effect of palladium nanosheets. The temperature versus time plots were recorded for various concentrations of palladium nanosheets (edge length, 41 nm) on irradiation by a 1 W laser. , Viability of healthy liver cells incubated for 48 h with different concentrations of palladium nanosheets. , Viability of human hepatoma cells upon irradiation by an 808 nm laser with a power density of 1.4 W cm−2 for various periods. Before irradiation, the cells were incubated with palladium nanosheets (20 µg ml−1) for 12 h. Cell viabilities were measured by standard MTT assay. ,, Micrographs corresponding to 2 min () and 5 min () irradiation. Dead cells are stained with trypan blue. Error bars in and are the standard deviations of the means of five independent determinations. Scale bars, 50 µm. * Figure 4: Comparison of electrocatalytic properties of palladium nanosheets and palladium black. The CV curves were recorded in an aqueous solution containing 0.5 M H2SO4 and 0.25 M HCOOH at a scan rate of 50 mV s−1. Edge size of palladium nanosheets, 41 nm; palladium black from Aldrich (47 m2 g−1). Author information * Abstract * Author information * Supplementary information Affiliations * State Key Laboratory for Physical Chemistry of Solid Surfaces and Department of Chemistry, College of Chemistry and Chemical Engineering, Xiamen University, Xiamen 361005, China * Xiaoqing Huang, * Shaoheng Tang, * Xiaoliang Mu, * Yan Dai, * Guangxu Chen, * Zhiyou Zhou & * Nanfeng Zheng * Department of Physics, Xiamen University, Xiamen 361005, China * Fangxiong Ruan & * Zhilin Yang Contributions X.Q.H. performed the experiments, collected and analysed the data, and wrote the paper. S.H.T. carried out the apoptosis assay and in vitro photothermal therapy tests. X.L.M. was responsible for AFM analysis. Y.D. and G.X.C. helped with synthesis of the materials. Z.Y.Z. helped with the electrochemical and FTIR measurements. F.X.R. and Z.L.Y. carried out the calculations of extinction spectra. N.F.Z. conceived the experiments, planned the synthesis, analysed the results and wrote the paper. Competing financial interests The authors declare no competing financial interests. Corresponding author Correspondence to: * Nanfeng Zheng Supplementary information * Abstract * Author information * Supplementary information PDF files * Supplementary information (3,422 KB) Supplementary information Additional data
  • Vibrational and electronic heating in nanoscale junctions
    - UNKNOWN 6(1):33-38 (2011)
    Nature Nanotechnology | Letter Vibrational and electronic heating in nanoscale junctions * Daniel R. Ward1 Search for this author in: * NPG journals * PubMed * Google Scholar * David A. Corley2 Search for this author in: * NPG journals * PubMed * Google Scholar * James M. Tour2 Search for this author in: * NPG journals * PubMed * Google Scholar * Douglas Natelson1, 3 Contact Douglas Natelson Search for this author in: * NPG journals * PubMed * Google Scholar * Affiliations * Contributions * Corresponding authorJournal name:Nature NanotechnologyVolume: 6,Pages:33–38Year published:(2011)DOI:doi:10.1038/nnano.2010.240Received23 July 2010Accepted08 November 2010Published online12 December 2010 Abstract * Abstract * Author information * Supplementary information Article tools * Full text * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg Understanding and controlling the flow of heat is a major challenge in nanoelectronics. When a junction is driven out of equilibrium by light or the flow of electric charge, the vibrational and electronic degrees of freedom are, in general, no longer described by a single temperature1, 2, 3, 4, 5, 6. Moreover, characterizing the steady-state vibrational and electronic distributions in situ is extremely challenging. Here, we show that surface-enhanced Raman emission may be used to determine the effective temperatures for both the vibrational modes and the electrons in the current in a biased metallic nanoscale junction decorated with molecules7. Molecular vibrations show mode-specific pumping by both optical excitation8 and d.c. current9, with effective temperatures exceeding several hundred kelvin. Anti-Stokes electronic Raman emission10, 11 indicates that the effective electronic temperature at bias voltages of a few hundred millivolts can reach values up to three times the! values measured when there is no current. The precise effective temperatures are model-dependent, but the trends as a function of bias conditions are robust, and allow direct comparisons with theories of nanoscale heating. View full text Subject terms: * Electronic properties and devices Figures at a glance * Figure 1: Measurement overview. , SEM false-colour image of a typical nanogap. , Schematic of electrical and optical measurements. , Waterfall plot showing the Raman response of an OPV3 junction (in CCD counts) as a function of d.c. bias V (y-axis) and Raman shift (x-axis). The anti-Stokes spectrum (left) shows a strong dependence on V, whereas the Stokes spectrum (right) is relatively constant as a function of V. The strong Stokes peak at 520 cm−1 is from the silicon substrate. Note, the false-colour scales for Stokes and anti-Stokes signals are different. , Current (top) and differential conductance (bottom) measured simultaneously as a function of V. * Figure 2: Optically driven vibrational pumping. , Raman response of a dodecanethiol-coated junction (in CCD counts; see false-colour bars) as a function of time (y-axis) and Raman shift (x-axis) under zero bias. Note, the false-colour scales for Stokes and anti-Stokes signals are different. The junction switches stochastically between several stable configurations, each with characteristic spectra that exhibit strong optical pumping of vibrational modes at 1,099 cm−1 (C–C stretch) and 1,475 cm−1 (CH2 or CH3 deformation). , Spectra from specific time slices in . Note that the higher energy peak spectrally diffuses between 1,475 cm−1 and 1,525 cm−1 and the lower energy peak between 1,099 cm−1 and 1,110 cm−1. The temperature of the 1,099 cm−1 mode changes as follows with increasing time: 769 K, 1,722 K, 532 K, 754 K, 512 K and 775 K. The temperature of the 1,475 cm−1 mode changes as follows: 701 K, 815 K, 658 K, 729 K, 648 K and 746 K. Note that at 70 s, a vibration at 1,450 cm−1 is observed at 2,161 K. A! ll temperatures have an uncertainty of ±10 K. , Power dependence of Stokes (black symbols) and anti-Stokes (blue symbols) signal taken from a different device, also showing optical pumping. As expected, in the optical pumping regime the Stokes signal is linear (solid black line) in laser power, whereas the anti-Stokes signal increases quadratically (solid blue line) in laser power. Error bars indicate uncertainty in the signal due to read and shot noise in the CCD. * Figure 3: Electrically driven vibrational pumping. , Effective vibrational temperature as a function of V for two OPV3 modes: 1,317 cm−1 (red) and 1,625 cm−1 (blue). Error bars indicate uncertainty in temperature due to anti-Stokes amplitude measurements. Inset: I–V curve for this device. , Raman response of this device as a function of V (y-axis) and Raman shift (x-axis). Note, the false-colour scales for the Stokes and anti-Stokes signals are different. , Sample Raman spectra at six different bias voltages. The full scale of the anti-Stokes signal is 235 counts; the full scale of the Stokes signal is 10,000 counts. , Effective vibrational temperature as a function of V for three OPV3 modes: 1,815 cm−1 (black), 1,480 cm−1 (red) and 562 cm−1 (blue). Error bars indicate uncertainty in temperature due to anti-Stokes amplitude measurements. Simultaneous optical and electrical vibrational pumping are observed for the 1,810 cm−1 mode as Teff is much greater than 80 K at V = 0. , Raman response of this device as a fu! nction of V (y-axis) and Raman shift (x-axis). Note, the false-colour scales for Stokes and anti-Stokes signals are different. , Sample Raman spectra at six different bias voltages. The full scale of the anti-Stokes signal is 350 counts; the full scale of the Stokes signal is 10,000 counts. * Figure 4: Electronic heating under bias. , Effective temperature (blue; left axis) and dissipated electrical power (red; right axis) versus bias voltage V in a nominally bare device. Error bars are described in the text. Inset: current/voltage curves for this device. Error bars are described in the text. ,, Raman response shown as a Raman signal (in CCD counts) as a function of voltage and Raman shift (), and as the Raman intensity (in CCD counts) as a function of Raman shift () at three different voltages (blue lines); the green lines are best fits to the data given by equation (2). Only the anti-Stokes signals are shown in and . This device shows no molecular Raman peaks, and is considered a 'clean' junction. –, The same data for the OPV3 device used for Figs 1 and 3. The data in ,, demonstrate that bias-driven electronic heating is also detectable in junctions that show optical pumping and bias-driven vibrational heating. Author information * Abstract * Author information * Supplementary information Affiliations * Department of Physics and Astronomy, Rice University, 6100 Main Street, Houston, Texas 77005, USA * Daniel R. Ward & * Douglas Natelson * Department of Chemistry, Rice University, 6100 Main Street, Houston, Texas 77005, USA * David A. Corley & * James M. Tour * Department of Electrical and Computer Engineering, Rice University, 6100 Main Street, Houston, Texas 77005, USA * Douglas Natelson Contributions D.R.W. fabricated the devices, performed all measurements, and analysed the data. D.N. supervised and provided continuous guidance for the experiments and the analysis. D.A.C. synthesized the OPV3 molecules under the supervision of J.M.T. The bulk of the paper was written by D.R.W. and D.N. All authors discussed the results and contributed to manuscript revision. Competing financial interests The authors declare no competing financial interests. Corresponding author Correspondence to: * Douglas Natelson Supplementary information * Abstract * Author information * Supplementary information PDF files * Supplementary information (2,043 KB) Supplementary information Additional data
  • Nanoparticle-induced unfolding of fibrinogen promotes Mac-1 receptor activation and inflammation
    - UNKNOWN 6(1):39-44 (2011)
    Nature Nanotechnology | Letter Nanoparticle-induced unfolding of fibrinogen promotes Mac-1 receptor activation and inflammation * Zhou J. Deng1 Search for this author in: * NPG journals * PubMed * Google Scholar * Mingtao Liang2, 3 Search for this author in: * NPG journals * PubMed * Google Scholar * Michael Monteiro4 Search for this author in: * NPG journals * PubMed * Google Scholar * Istvan Toth2, 3 Search for this author in: * NPG journals * PubMed * Google Scholar * Rodney F. Minchin1 Contact Rodney F. Minchin Search for this author in: * NPG journals * PubMed * Google Scholar * Affiliations * Contributions * Corresponding authorJournal name:Nature NanotechnologyVolume: 6,Pages:39–44Year published:(2011)DOI:doi:10.1038/nnano.2010.250Received23 September 2010Accepted16 November 2010Published online19 December 2010 Abstract * Abstract * Author information * Supplementary information Article tools * Full text * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg The chemical composition, size, shape and surface characteristics of nanoparticles affect the way proteins bind to these particles, and this in turn influences the way in which nanoparticles interact with cells and tissues1, 2, 3, 4, 5. Nanomaterials bound with proteins can result in physiological and pathological changes, including macrophage uptake1, 6, blood coagulation7, protein aggregation8 and complement activation7, 9, but the mechanisms that lead to these changes remain poorly understood. Here, we show that negatively charged poly(acrylic acid)-conjugated gold nanoparticles bind to and induce unfolding of fibrinogen, which promotes interaction with the integrin receptor, Mac-1. Activation of this receptor increases the NF-κB signalling pathway, resulting in the release of inflammatory cytokines. However, not all nanoparticles that bind to fibrinogen demonstrated this effect. Our results show that the binding of certain nanoparticles to fibrinogen in plasma offers an! alternative mechanism to the more commonly described role of oxidative stress in the inflammatory response to nanomaterials. View full text Subject terms: * Nanomedicine * Nanoparticles Figures at a glance * Figure 1: Fibrinogen is the major human plasma protein bound by PAA–GNP. , SDS–PAGE of human plasma proteins bound to PAA–GNP with diameters of 5, 10 and 20 nm. Three major protein bands were observed at ~65, 55 and 45 kDa. , Unbound fibrinogen following pull-down with PAA–GNP with diameters of ~5 nm (blue) or 20 nm (red). Purified fibrinogen (0.6 µg) was incubated with increasing amounts of PAA–GNP. Inset: unbound fibrinogen is plotted against total surface area for the two nanoparticles. , Crystal structure of fibrinogen. The protein was drawn using Swiss-PdbViewer and coordinates for PDB entry 3GHG. Common domains are shown. Inset: the C-terminus of the γ chain (purple) that interacts with the Mac-1 receptor. , Circular dichroism of fibrinogen in the absence and presence of increasing concentrations of 5 nm PAA–GNP. * Figure 2: Selective binding of fibrinogen/PAA–GNP complexes to Mac-1 receptors. , HL-60 cells are Mac-1-receptor-negative cells, as shown by flow cytometry following labelling with fluorescent CD11b antibodies (upper panel, solid lines) and THP-1 cells are Mac-1-receptor-positive. This was confirmed by plating both HL-60 and THP-1 cells onto immobilized fibrinogen (Supplementary Fig. S4). Lower panel shows binding of fibrinogen alone (open bars) or fibrinogen with 5 nm PAA–GNP (filled bars) to THP-1 cells and HL-60 is shown. Addition of nanoparticles significantly increased the binding to THP-1 cells but not to HL-60 cells. Replacing fibrinogen with albumin abrogated the effect of the nanoparticles. Results are mean ± s.e.m, n = 3; asterisk indicates P < 0.05. , HEK293 cells were transfected with empty vector (EV) or CD11b/CD18 constructs and Mac-1 receptor expression was determined by flow cytometry (upper panels). Lower panel shows binding of fibrinogen alone (open bars) or fibrinogen with 5 nm PAA–GNP (filled bars) is shown. The nanoparticles in! creased fibrinogen binding in Mac-1-receptor-positive cells only. Results are mean ± s.e.m., n = 3; asterisk indicates P < 0.05. , PAA–GNP (20 nm) did not induce fibrinogen binding to THP-1 cells to the same extent as the 5 nm. Binding was performed with an equal surface area (3,900 mm2) for each of the nanoparticles to ensure similar protein binding. , Pre-treatment of THP-1 cells with the P2 peptide significantly reduced the binding of fibrinogen in the presence of 5 nm PAA–GNP (grey bars). Control peptide, H19, showed no inhibitory effects on binding (filled bars). Results are mean ± s.e.m., n = 3. , PAA–GNP (20 nm) induced fibrinogen binding to THP-1 cells when the level of protein binding was reduced. However, no increase in binding was seen under the same conditions in HL-60 cells. Percent binding saturation is shown on the x-axis and was determined from the data shown in Fig. 1b. Results are mean ± s.e.m., n = 3, expressed as a percentage of the control (100! %). , Electrophoretic mobility shift assay, showing the increa! sed nuclear localization of NF-κB in THP-1 cells when exposed to the fibrinogen/PAA–GNP complexes. The open arrow indicates the location of the P65 complex of NF-κB, which was confirmed by a supershift (solid arrow) with anti-P65 antibody (lane 5). * Figure 3: Pro-inflammatory effects of fibrinogen/PAA–GNP complexes. ,, Treatment of THP-1 cells with complexes of fibrinogen (33 µg ml−1) and 5 nm PAA–GNP (100 µg ml−1) induced the secretion of IL-8 () and TNF-α (). Neither fibrinogen alone nor PAA–GNP altered cytokine release. The concentration effect of the complexes on cytokine release is shown in Supplementary Fig. S5. NF-κB pathway inhibitor, Bay 11-7082, inhibited the secretion of both cytokines. Lipopolysaccharide-treated cells were used as a positive control. Results are mean ± s.e.m., n = 3. Single asterisk indicates P < 0.05 compared to control (no treatment). Double asterisk indicates P < 0.05 compared to respective treatments without Bay 11-7082. ,, THP-1 cells treated with 20 nm PAA–GNP bound to excess fibrinogen did not induce IL-8 () or TNF-α () release. Nanoparticles were adjusted to equal total surface area for similar protein binding. ,, Cells treated with 20 nm PAA–GNP bound to a reduced concentration of fibrinogen (10 µg ml−1), which resulted in only ! 33% binding saturation, induced low but significant release of IL-8 () and a more substantial release of TNF-α (). Nanoparticles (5 nm; 30 µg ml−1) bound to 10 µg ml−1 fibrinogen are shown for comparison. Asterisk indicates P < 0.05 compared to nanoparticles alone (respective controls). * Figure 4: Effects of nanoparticle surface characteristics on fibrinogen binding. , Unbound fibrinogen following pull-down with PAA–PDHA–GNP. Purified fibrinogen (0.6 µg) was incubated with 2 µg of each nanoparticle. Only the 100% PAA/0% PDHA–GNP and 80% PAA/20% PDHA–GNP significantly bound fibrinogen. , Binding of fibrinogen to THP-1 cells was only significantly increased with the nanoparticles containing 100% PAA. Results are mean ± s.e.m., n = 3. Asterisk indicates P < 0.05 compared to control (no treatment). , Binding of fibrinogen to nano-metal oxides was determined by ultracentrifugation after mixing 0.6 µg protein with 8 µg nanoparticles. All the metal-oxide nanoparticles bound more than 70% of the fibrinogen. , Binding of the fibrinogen–metal oxide complexes to THP-1 cells was determined. Results are mean ± s.e.m., n = 3. Asterisk indicates P < 0.05 compared to control (no treatment). , Pre-treatment of THP-1 cells with the P2 peptide significantly reduced (P < 0.05) the binding of fibrinogen in the presence of nano-SiO2. Control p! eptide, H19, showed no inhibitory effect on the binding. Results are mean ± s.e.m., n = 3. Author information * Abstract * Author information * Supplementary information Affiliations * School of Biomedical Sciences, University of Queensland, Brisbane 4072, Australia * Zhou J. Deng & * Rodney F. Minchin * School of Chemistry and Molecular Biosciences, University of Queensland, Brisbane 4072, Australia * Mingtao Liang & * Istvan Toth * School of Pharmacy, University of Queensland, Brisbane 4072, Australia * Mingtao Liang & * Istvan Toth * Australian Institute for Bioengineering and Nanotechnology, University of Queensland, Brisbane 4072, Australia * Michael Monteiro Contributions Z.J.D. performed all the biological experiments, assisted in designing the biological experiments and co-wrote the manuscript. M.L. synthesized and characterized the nanoparticles. M.M. and I.T. designed the nanoparticle synthesis procedure. R.F.M. conceived and designed the biological studies and co-wrote the manuscript. Competing financial interests The authors declare no competing financial interests. Corresponding author Correspondence to: * Rodney F. Minchin Supplementary information * Abstract * Author information * Supplementary information PDF files * Supplementary information (1,298 KB) Supplementary information Additional data
  • Large intrinsic energy bandgaps in annealed nanotube-derived graphene nanoribbons
    - UNKNOWN 6(1):45-50 (2011)
    Nature Nanotechnology | Article Large intrinsic energy bandgaps in annealed nanotube-derived graphene nanoribbons * T. Shimizu1 Search for this author in: * NPG journals * PubMed * Google Scholar * J. Haruyama1 Contact J. Haruyama Search for this author in: * NPG journals * PubMed * Google Scholar * D. C. Marcano2 Search for this author in: * NPG journals * PubMed * Google Scholar * D. V. Kosinkin2 Search for this author in: * NPG journals * PubMed * Google Scholar * J. M. Tour2 Contact J. M. Tour Search for this author in: * NPG journals * PubMed * Google Scholar * K. Hirose3 Search for this author in: * NPG journals * PubMed * Google Scholar * K. Suenaga3 Search for this author in: * NPG journals * PubMed * Google Scholar * Affiliations * Contributions * Corresponding authorsJournal name:Nature NanotechnologyVolume: 6,Pages:45–50Year published:(2011)DOI:doi:10.1038/nnano.2010.249Received14 October 2010Accepted12 November 2010Published online19 December 2010 Abstract * Abstract * Author information * Supplementary information Article tools * Full text * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg The usefulness of graphene for electronics has been limited because it does not have an energy bandgap. Although graphene nanoribbons have non-zero bandgaps, lithographic fabrication methods introduce defects that decouple the bandgap from electronic properties, compromising performance. Here we report direct measurements of a large intrinsic energy bandgap of ~50 meV in nanoribbons (width, ~100 nm) fabricated by high-temperature hydrogen-annealing of unzipped carbon nanotubes. The thermal energy required to promote a charge to the conduction band (the activation energy) is measured to be seven times greater than in lithographically defined nanoribbons, and is close to the width of the voltage range over which differential conductance is zero (the transport gap). This similarity suggests that the activation energy is in fact the intrinsic energy bandgap. High-resolution transmission electron and Raman microscopy, in combination with an absence of hopping conductance and stoc! hastic charging effects, suggest a low defect density. View full text Subject terms: * Electronic properties and devices * Synthesis and processing Figures at a glance * Figure 1: Characterization of graphene nanoribbons. , Field-emission SEM image of an ensemble of the as-grown nanoribbons, which were dispersed on a silicon oxide substrate in a water droplet containing a suspension of nanoribbons. The nanoribbons are entangled and not sufficiently exfoliated. Insets (right): atomic force microscopy images of individual nanoribbons spread by applying a strong air flow to the droplet (see Methods). Inset (left): height of the nanoribbon measured along the longitudinal direction. The thickness of ~0.8 nm indicates a single-layer nanoribbon. , HRTEM image of the as-grown nanoribbon (no annealing; see Methods), showing a clear hexagonal lattice of graphene with few defects and some oxidized parts. Annealing (see Methods) strongly enhances the quality of the nanoribbons and also results in carrier doping. , Typical Raman spectrum of an annealed bilayer nanoribbon taken with a laser excitation of 532 nm and 0.14 mW incident power at room temperature. The width of the nanoribbon is ~100 nm and the G! /D band ratio is as high as ~2.2. , FET fabricated using a nanoribbon end-bonded by two metal electrodes, which eliminates single-electron charging effects (see Supplementary Section 1). The thickness of the SiO2 layer on the gold/titanium backgate electrode was 300 nm, and the spacing of source and drain electrodes was 500 nm in all samples. * Figure 2: Electronic characteristics of a graphene-nanoribbon FET. , Typical drain current (ISD) versus drain voltage (VSD) relationship for a sample (W = 75 nm and N = 1) at room temperature (inset) and T = 1.5 K (main panel), revealing a strong zero-bias (G0) anomaly with a voltage width of ΔVSD ≈ ± V, even at a backgate voltage (VBG) of ±20 V. ΔVSD was determined from the VSD range for differential conductance (dISD/dVSD) ≈ 0. The temperature dependence of the G0 anomaly does not follow the formula for single-electron charging effect26, 27. This is consistent with end-bonding of the nanoribbon. , Differential conductance (dISD/dVSD) as a function of VBG at T = 1.5 K for the sample in . A transport gap of the backgate voltage of ΔVBG ≈ 1 V is observed. At higher VSD, the gap becomes ambiguous (Fig. 3). In contrast, at lower VSD, the same gap was observed in most cases, although it also becomes ambiguous due to insulating behaviour at values of VBG outside the gap. The energy estimated from this in the single-particle energy spe! ctrum, Δm, is ~70 meV, which is smaller than that for lithographically formed nanoribbons (~100 meV) with the same W. * Figure 3: Source–drain current versus backgate voltage. –, IDS versus VBG in four different nanoribbon FETs. VSD was changed in steps of 1 V. A significant increase in ISD in the −VBG region suggests hole-dominant transport. The ratio of ISD at VBG = –20 V to the minimum ISD strongly depends on VSD, and becomes large for large absolute values of VSD. This suggests the appearance of different states driven by high VSD (such as edge reconstruction; Supplementary Section 7). The transport gap and slight ambipolar feature shown in Fig. 2b remain at low VSD (~1 V) in . (W, width (nm); N, number of layers.). * Figure 4: Temperature dependence of minimum conductance around the charge neutrality point and activation energy. , Arrhenius plot for minimum conductance (Gmin) versus temperature of the samples shown in Fig. 3. Gmin represents the values at the charge neutrality point (VBG ≈ 0–2 V). An Ea of ~50 meV was obtained from the dotted lines, and Gmin ∝ exp(−Ea/2kBT) at high temperatures is mostly independent of W and N, except for the W = 75 nm sample, where Ea increases slightly to ~55 meV. This value is seven times greater than those in lithographically formed nanoribbons and is close to the Δm value (~80%). , Ea and Δm values as a function of W for two different values of N. The trend in is more evident. * Figure 5: Single-electron spectroscopy—half part of a Coulomb diamond measured at T = 1.5 K. The colours represent differential conductance. ΔVBG is 5 mV. The transport gap is represented by the region of 20 × 10−12 S. No stochastic Coulomb diamonds can be observed inside the transport gap (Supplementary Section 1). A transport gap only exists around the charge neutrality point. The measured sample, with W = 80 nm and N = 1, is different from that in Figs 2 and 3. Author information * Abstract * Author information * Supplementary information Affiliations * Faculty of Science and Engineering, Aoyama Gakuin University, 5-10-1 Fuchinobe, Sagamihara, Kanagawa 252-5258, Japan * T. Shimizu & * J. Haruyama * Department of Chemistry and Mechanical Engineering and Materials Science, Rice University, 6100 Main Street, Houston, Texas 77005, USA * D. C. Marcano, * D. V. Kosinkin & * J. M. Tour * Nanotube Research Center, National Institute of Advanced Industrial Science and Technology (AIST), AIST Central 5, Tsukuba, 305-8565, Japan * K. Hirose & * K. Suenaga Contributions J.H., J.M.T. and K.S conceived and designed the experiments. T.S., D.C.M., D.V.K., and K.H. performed the experiments. J.H. analysed the data. J.H. and J.M.T. co-wrote the paper. Competing financial interests The authors declare no competing financial interests. Corresponding authors Correspondence to: * J. Haruyama or * J. M. Tour Supplementary information * Abstract * Author information * Supplementary information PDF files * Supplementary information (814 KB) Supplementary information Additional data
  • Single-walled carbon nanotubes as excitonic optical wires
    - UNKNOWN 6(1):51-56 (2011)
    Nature Nanotechnology | Article Single-walled carbon nanotubes as excitonic optical wires * Daniel Y. Joh1, 2, 4 Search for this author in: * NPG journals * PubMed * Google Scholar * Jesse Kinder2, 4 Search for this author in: * NPG journals * PubMed * Google Scholar * Lihong H. Herman1, 4 Search for this author in: * NPG journals * PubMed * Google Scholar * Sang-Yong Ju2 Search for this author in: * NPG journals * PubMed * Google Scholar * Michael A. Segal2 Search for this author in: * NPG journals * PubMed * Google Scholar * Jeffreys N. Johnson2 Search for this author in: * NPG journals * PubMed * Google Scholar * Garnet K.-L. Chan2 Search for this author in: * NPG journals * PubMed * Google Scholar * Jiwoong Park2, 3 Contact Jiwoong Park Search for this author in: * NPG journals * PubMed * Google Scholar * Affiliations * Contributions * Corresponding authorJournal name:Nature NanotechnologyVolume: 6,Pages:51–56Year published:(2011)DOI:doi:10.1038/nnano.2010.248Received25 October 2010Accepted12 November 2010Published online19 December 2010 Abstract * Abstract * Author information * Supplementary information Article tools * Full text * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg Although metallic nanostructures are useful for nanoscale optics, all of their key optical properties are determined by their geometry. This makes it difficult to adjust these properties independently, and can restrict applications. Here we use the absolute intensity of Rayleigh scattering to show that single-walled carbon nanotubes can form ideal optical wires. The spatial distribution of the radiation scattered by the nanotubes is determined by their shape, but the intensity and spectrum of the scattered radiation are determined by exciton dynamics, quantum-dot-like optical resonances and other intrinsic properties. Moreover, the nanotubes display a uniform peak optical conductivity of ~8 e2/h, which we derive using an exciton model, suggesting universal behaviour similar to that observed in nanotube conductance. We further demonstrate a radiative coupling between two distant nanotubes, with potential applications in metamaterials and optical antennas. View full text Subject terms: * Carbon nanotubes and fullerenes * Photonic structures and devices Figures at a glance * Figure 1: Optical scattering from single-walled carbon nanotubes. , Upper panel: schematic illustrating electromagnetic radiation from a long, straight wire. Intensity plot corresponds to the strength of the scattered electric field (Escatt), which decays as 1/√r. Middle panel: schematic of an electronic band diagram for a semiconducting nanotube (where kz represents the azimuthal quantum number). An interband transition from valence to conduction band (red arrow) resulting from optical excitation leads to the formation of an excitonic bound state that dissociates into free particles in lower sub-bands at rate ΓX (dashed blue arrows). Lower panel: optical excitation and exciton formation (e–h) in a nanotube by an electromagnetic plane wave (Eex). The solid arrow indicates the direction of propagation of the incident photons. , Representative spatial Rayleigh image, showing more than 10 nanotubes simultaneously (in false colour, corresponding to strongly scattered wavelengths). , Optical setup schematic. The incident electric field Eex! is linearly polarized and incident at angle θex with respect to the nanotube axis, inducing a surface current I along the nanotube. The scattered light is focused onto a disk or cone around the nanotube axis and is collected with a detection angle θdet = 80.6°. The Fraunhofer image is effectively obtained by removing the tube lens (TL) and placing the CCD immediately after the objective lens (OL) to image the nanotube radiation pattern, as indicated by the dotted blue line (see Supplementary Information). ,, Main panels: radiation behaviour for nanotubes. Spatial Rayleigh images (upper inset) and radiation patterns from Fraunhofer imaging (lower inset) of individual nanotubes when θex = 90° () and when θex ≠ 90 (). * Figure 2: Scattering patterns for periodically spaced nanotube segments. , Colour Rayleigh image before (upper panel) and after (lower panel) cutting. Scale bar, 5 µm. , Rayleigh spectra (normalized to the peak) before and after patterning for the nanotube marked by the symbols in , Schematic illustrating the scattering pattern for periodically spaced (h = pitch distance) linear structures. , Upper panel: Fraunhofer image for a nanotube with h = 2.0 µm after cutting. Lower panel: measured scattering patterns for nanotubes of different pitch sizes after cutting. Asterisks denote side bands depicted in . * Figure 3: Frequency-dependent scattering intensity and optical conductivity of single-walled carbon nanotubes. , Colour Rayleigh images of five nanotubes, together with their corresponding resonant Rayleigh peaks and diameters determined by AFM (height traces shown in red). , Normalized spatial Rayleigh scattering intensity plots for tubes of different diameter (dexp) measured at their respective resonance energies. , √(δscattλ) as a function of dexp, measured for 19 nanotube resonances of various sub-band transitions. Inset: histogram of peak dynamic conductivity |σ|peak in units of G0 (e2/h). , Main panel: calculated plots of Re[σ(ω)], Im[σ(ω)] and |σ(ω)| versus ħω for a representative semiconducting nanotube using the exciton model. Inset: calculated values of |σ|peak for different resonances and nanotube diameters using the exciton model (same symbols as in ). * Figure 4: Radiative coupling between distant single-walled carbon nanotubes. , AFM image of two nanotubes with overlapping spectral resonances centred at 634 nm (λL) and 664 nm (λR) (for nanotubes L and R, respectively). The two nanotubes run parallel to each other over a distance of 10 µm. Corresponding height traces are shown in red. , Main panels: optical coupling (insets show spatial Rayleigh images near the coupling region, denoted by blue lines) recorded at 634 and 664 nm. Re[σ(ω)] represented by solid lines and Im[σ(ω)] by dashed lines. Scale bar, 5 µm. , Rayleigh scattering intensity contour of excitation wavelength versus position for the green cross-sections marked in the inset of for coupled (middle panel) and uncoupled (left and right panels) regions. , Intensity contributions for nanotubes L and R in the uncoupled and coupled regions obtained from Gaussian deconvolution (left inset) of . Inset: calculated values for the observed transition. Arrows indicate the changes in the scattering intensity of tube R before and after intertu! be coupling. Author information * Abstract * Author information * Supplementary information Primary authors * These authors contributed equally to this work * Daniel Y. Joh, * Jesse Kinder & * Lihong H. Herman Affiliations * School of Applied and Engineering Physics, Cornell University, Ithaca, New York 14853, USA * Daniel Y. Joh & * Lihong H. Herman * Department of Chemistry and Chemical Biology, Cornell University, Ithaca, New York 14853, USA * Daniel Y. Joh, * Jesse Kinder, * Sang-Yong Ju, * Michael A. Segal, * Jeffreys N. Johnson, * Garnet K.-L. Chan & * Jiwoong Park * Kavli Institute at Cornell for Nanoscale Science, Cornell University, Ithaca, New York 14853, USA * Jiwoong Park Contributions D.J. and L.H. performed optical measurements and analysed the data. J.K. carried out theoretical calculations. S.-Y.J. and J.J. performed Raman spectroscopy measurements. M.S. carried out nanotube synthesis. G.C. and J.P. supervised the project. Competing financial interests The authors declare no competing financial interests. Corresponding author Correspondence to: * Jiwoong Park Supplementary information * Abstract * Author information * Supplementary information PDF files * Supplementary information (1,061 KB) Supplementary information Additional data
  • Multifunctional carbon-nanotube cellular endoscopes
    - UNKNOWN 6(1):57-64 (2011)
    Nature Nanotechnology | Article Multifunctional carbon-nanotube cellular endoscopes * Riju Singhal1, 5 Search for this author in: * NPG journals * PubMed * Google Scholar * Zulfiya Orynbayeva1, 2, 5 Search for this author in: * NPG journals * PubMed * Google Scholar * Ramalingam Venkat Kalyana Sundaram3, 5 Search for this author in: * NPG journals * PubMed * Google Scholar * Jun Jie Niu1, 5 Search for this author in: * NPG journals * PubMed * Google Scholar * Sayan Bhattacharyya1, 5, 6 Search for this author in: * NPG journals * PubMed * Google Scholar * Elina A. Vitol4, 5 Search for this author in: * NPG journals * PubMed * Google Scholar * Michael G. Schrlau1, 5 Search for this author in: * NPG journals * PubMed * Google Scholar * Elisabeth S. Papazoglou3, 5 Search for this author in: * NPG journals * PubMed * Google Scholar * Gary Friedman4, 5 Contact Gary Friedman Search for this author in: * NPG journals * PubMed * Google Scholar * Yury Gogotsi1, 5 Contact Yury Gogotsi Search for this author in: * NPG journals * PubMed * Google Scholar * Affiliations * Contributions * Corresponding authorsJournal name:Nature NanotechnologyVolume: 6,Pages:57–64Year published:(2011)DOI:doi:10.1038/nnano.2010.241Received31 August 2010Accepted09 November 2010Published online12 December 2010 Abstract * Abstract * Author information * Supplementary information Article tools * Full text * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg Glass micropipettes, atomic force microscope tips and nanoneedles can be used to interrogate cells, but these devices either have conical geometries that can damage cells during penetration or are incapable of continuous fluid handling. Here, we report a carbon-nanotube-based endoscope for interrogating cells, transporting fluids and performing optical and electrochemical diagnostics at the single organelle level. The endoscope, which is made by placing a multiwalled carbon nanotube (length, 50–60 µm) at the tip of a glass pipette, can probe the intracellular environment with a spatial resolution of ~100 nm and can also access organelles without disrupting the cell. When the nanotube is filled with magnetic nanoparticles, the endoscope can be remotely manoeuvered to transport nanoparticles and attolitre volumes of fluids to and from precise locations. Because they are mounted on conventional glass micropipettes, the endoscopes readily fit standard instruments, creating a ! broad range of opportunities for minimally invasive intracellular probing, drug delivery and single-cell surgery. View full text Subject terms: * Carbon nanotubes and fullerenes * Nanobiotechnology * Nanosensors and other devices Figures at a glance * Figure 1: Comparison between cellular endoscopes and glass pipettes. , Schematic showing a conventional glass pipette (left) and a nanotube endoscope (right) interrogating cells. , Schematic of the nanotube endoscope. A multiwalled carbon nanotube is attached to the end of a glass pipette, which is coated with a non-conducting epoxy on the outside and a conducting epoxy on the inside. , A HeLa cell (left) being injected by a 1 µm commercial glass pipette, and a primary rat hepatocyte nucleus (right) being interrogated by a 100 nm nanotube endoscope. ,, Scanning electron micrograph of as-assembled endoscopes with 100 and 50 nm carbon nanotube tips, respectively. Inset in : nanotube tip opening. Epoxy glue seals the glass pipette entrance, and the ends of the nanotube remain open for fluid transfer. , Optical image of a glass pipette with a carbon-nanotube tip (not visible at this magnification). * Figure 2: Mechanical robustness, flexibility and remote manipulation of the nanotube endoscope. ,, Differential interference contrast micrographs showing a 100 nm nanotube tip of the endoscope bending (left) and elastically recovering its shape (right) when pushed against a cell membrane () or a glass slide (). , Sequential optical micrographs of a nanotube tip bending towards a magnetic field (white arrow). Superparamagnetic properties and flexibility of the nanotube tip allow remote magnetic manipulation. * Figure 3: Fluid and particulate flow through the nanotube endoscope. , Optical micrographs showing the transport of an oil-based ferrofluid-fluorescent dye under an applied magnetic field. Inset: schematic of the fluid-filled nanotube endoscope ejecting fluid at its tip. , Optical micrograph showing the flow and alighment of 50 nm polypropylene particles (green spheres) inside a carbon-nanotube tip. ,, Fluorescence () and differential interference contrast () micrographs showing a cell being interrogated with an endoscope filled with FITC-labelled (green) fluorescent polymer nanoparticles. The fluorescence micrograph in shows mitochondria labelled with Mitotracker Orange (red). * Figure 4: Application of nanotube endoscopes for SERS and electrochemistry. , Schematic of a SERS-active endoscope consisting of a nanotube tip decorated with gold nanoparticles. , Transmission electron micrograph of the SERS-active nanotube tip. , Raman spectra recorded when the SERS-active endoscope tip is positioned inside (red spectrum) and outside (black spectrum) a HeLa cell. Inset: optical micrograph showing the corresponding 200-nm-diameter endoscope tip positioned in the cell cytoplasm. , Voltammetric traces obtained using the nanotube endoscope in 100 mM supporting electrolyte alone (circles) and 100 µM (triangles) and 1 mM (squares) potassium ferricyanide. Inset: oxidative current change as a function of potassium ferricyanide concentration. * Figure 5: Intracellular Ca2+ response to mechanical stimulation. ,, Differential interference contrast micrographs showing a 200-nm-tip diameter glass pipette tip () and a 200-nm-diameter endoscope tip () penetrating the cell membrane of a HeLa cell. ,, Pseudo-colour fluorescent images representing the cytosolic Ca2+ concentration corresponding to cell membrane penetration by the glass pipette () and endoscope (). The blue streak (arrow) in represents the aspiration of Ca2+-labelled cytosol into the endoscope after membrane penetration. , Typical Ca2+ response as a function of time upon insertion of a 200-nm-diameter glass pipette (blue trace) and 100-nm-diameter endoscope (red trace). * Figure 6: Effect of probe insertion on the cytoskeleton. ,, Differential interference contrast micrographs showing a HeLa cell before () and after () insertion of a conical glass pipette. ,, Corresponding fluorescent images of actin cytoskeleton before () and after () insertion of a glass pipette. The circled area in shows cytoskeletal destruction. , Differential interference contrast micrograph (,) and the corresponding fluorescent image (,) of the cell before (,) and after (,) insertion of a 100-nm-diameter endoscope. No damage or changes of the cell cytoskeleton were observed after insertion. The dotted circle in shows the point of insertion. Author information * Abstract * Author information * Supplementary information Affiliations * Department of Materials Science and Engineering, Drexel University, Philadelphia, Pennsylvania 19104, USA * Riju Singhal, * Zulfiya Orynbayeva, * Jun Jie Niu, * Sayan Bhattacharyya, * Michael G. Schrlau & * Yury Gogotsi * Department of Biochemistry and Molecular Biology, Drexel University, Philadelphia, Pennsylvania 19102, USA * Zulfiya Orynbayeva * School of Biomedical Engineering, Science and Health Systems, Drexel University, Philadelphia, Pennsylvania 19104, USA * Ramalingam Venkat Kalyana Sundaram & * Elisabeth S. Papazoglou * Department of Electrical and Computer Engineering, Drexel University, Philadelphia, Pennsylvania 19104, USA * Elina A. Vitol & * Gary Friedman * A.J. Drexel Nanotechnology Institute, Drexel University, Philadelphia, Pennsylvania 19104, USA * Riju Singhal, * Zulfiya Orynbayeva, * Ramalingam Venkat Kalyana Sundaram, * Jun Jie Niu, * Sayan Bhattacharyya, * Elina A. Vitol, * Michael G. Schrlau, * Elisabeth S. Papazoglou, * Gary Friedman & * Yury Gogotsi * Present address: Department of Chemical Sciences, Indian Institute of Science Education and Research, Kolkata, Mohanpur – 741252, Nadia, W.B., India * Sayan Bhattacharyya Contributions Y.G., G.F., E.P. and M.G.S. conceived the project and planned experiments. R.S. designed and fabricated the cellular endoscopes for all studies. Z.O. performed cell studies. R.S. and R.V.K.S. performed fluid and particulate flow studies. R.V.K.S. and M.G.S. carried out electrochemical studies. J.N., M.G.S. and E.V. performed SERS studies using the endoscopes. S.B. performed fluorescent labelling of the nanotubes. R.S., M.G.S., G.F. and Y.G. organized the manuscript, and all authors contributed to writing the manuscript. Competing financial interests The authors declare no competing financial interests. Corresponding authors Correspondence to: * Gary Friedman or * Yury Gogotsi Supplementary information * Abstract * Author information * Supplementary information PDF files * Supplementary information (1,417 KB) Supplementary information Additional data
  • Biomagnification of cadmium selenide quantum dots in a simple experimental microbial food chain
    - UNKNOWN 6(1):65-71 (2011)
    Nature Nanotechnology | Article Biomagnification of cadmium selenide quantum dots in a simple experimental microbial food chain * R. Werlin1, 2 Search for this author in: * NPG journals * PubMed * Google Scholar * J. H. Priester2, 3, 4 Search for this author in: * NPG journals * PubMed * Google Scholar * R. E. Mielke2, 3, 4, 5 Search for this author in: * NPG journals * PubMed * Google Scholar * S. Krämer6 Search for this author in: * NPG journals * PubMed * Google Scholar * S. Jackson2, 7 Search for this author in: * NPG journals * PubMed * Google Scholar * P. K. Stoimenov8 Search for this author in: * NPG journals * PubMed * Google Scholar * G. D. Stucky2, 6, 8 Search for this author in: * NPG journals * PubMed * Google Scholar * G. N. Cherr2, 7 Search for this author in: * NPG journals * PubMed * Google Scholar * E. Orias1 Search for this author in: * NPG journals * PubMed * Google Scholar * P. A. Holden2, 3, 4 Contact P. A. Holden Search for this author in: * NPG journals * PubMed * Google Scholar * Affiliations * Contributions * Corresponding authorJournal name:Nature NanotechnologyVolume: 6,Pages:65–71Year published:(2011)DOI:doi:10.1038/nnano.2010.251Received18 August 2010Accepted17 November 2010Published online19 December 2010 Abstract * Abstract * Author information * Supplementary information Article tools * Full text * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg Previous studies have shown that engineered nanomaterials can be transferred from prey to predator, but the ecological impacts of this are mostly unknown. In particular, it is not known if these materials can be biomagnified—a process in which higher concentrations of materials accumulate in organisms higher up in the food chain. Here, we show that bare CdSe quantum dots that have accumulated in Pseudomonas aeruginosa bacteria can be transferred to and biomagnified in the Tetrahymena thermophila protozoa that prey on the bacteria. Cadmium concentrations in the protozoa predator were approximately five times higher than their bacterial prey. Quantum-dot-treated bacteria were differentially toxic to the protozoa, in that they inhibited their own digestion in the protozoan food vacuoles. Because the protozoa did not lyse, largely intact quantum dots remain available to higher trophic levels. The observed biomagnification from bacterial prey is significant because bacteria are! at the base of environmental food webs. Our findings illustrate the potential for biomagnification as an ecological impact of nanomaterials. View full text Subject terms: * Electronic properties and devices * Surface patterning and imaging Figures at a glance * Figure 1: Extent and rate of growth of Tetrahymena varies with Pseudomonas prey treatment. , Tetrahymena population growth (filled symbols) and Pseudomonas population decline (open symbols) for control (triangles), CdSe QD (squares) and cadmium acetate (circles) treatments. Error bars represent standard error of the mean. For the Tetrahymena data, error bars are masked by the symbols. , Tetrahymena population increase for three individual cultures in the QD (squares) and cadmium acetate (circles) treatments. Tetrahymena cells that fed upon cadmium-acetate-grown bacteria stopped growing by 6 h, whereas those that fed on QD-grown bacteria continued to grow slowly for up to 14 h. * Figure 2: Tetrahymena cells after 24 h culture with Pseudomonas. –, Nomarski bright-field optical micrographs of Tetrahymena cells that have preyed on control (no cadmium) (), cadmium-acetate-grown () and CdSe QD-grown () Pseudomonas bacteria. Note the abnormally high accumulation of large food vacuoles (arrow) in . Some Pseudomonas cells can be seen in the media external to the Tetrahymena in all images. * Figure 3: Stunted digestion in Tetrahymena cells preying on CdSe QD-grown, but not cadmium-acetate-grown, Pseudomonas bacteria. –, Dark-field STEM images of Tetrahymena cells that have fed on control Pseudomonas (,), cadmium-acetate-grown bacteria (,) and CdSe QD-grown bacteria (,). ,, are taken at 1 h; is at 16 h, and , are at 24 h. Triangles, Pseudomonas cells; eFV and lFV, early and late food vacuoles; OA, oral apparatus; M and m, macronucleus and micronucleus. In , two eFV packed with undigested Pseudomonas cells are visible near the oral apparatus. Note the abundance of Pseudomonas outside the Tetrahymena cell. In , fine lamellar membranes (arrow) and intact Pseudomonas are seen in mid- to late-stage food vacuoles. A normal mitochondrion is also visible (star). In , the presence of an eFV at 1 h shows that normal phagocytic ingestion has occurred in cadmium acetate-grown Pseudomonas. In , intact Pseudomonas are found outside the Tetrahymena, and amorphous digestion products are seen in the lFV. Bright cadmium spots (arrow) appear throughout. In , eFV shows intact Pseudomonas, and lFV contains ! cellular debris, fine lamellar membranes and QDs (arrows). In , eFV (arrow) shows tightly packed, undigested Pseudomonas surrounded by numerous QDs. The observation of QDs throughout indicates that undigested QDs have crossed the food vacuole membrane. * Figure 4: CD:Se ratios obtained using EDS. Vertical lines represent the ranges of Cd:Se ratios. Boxes are bounded by the 75th and 25th percentiles; intermediate horizontal lines are data medians. The number of observations (100 nm2 spots) is located above each bar. The x-axis labels (left to right) include times relative to the time course of the trophic transfer experiments: as-synthesized CdSe QDs, washed CdSe QD-grown Pseudomonas (Pa) prey, endpoint CdSe QD-grown Pseudomonas outside the predator, endpoint Tetrahymena (Tt) food vacuole (FV) containing undigested CdSe QD-grown Pseudomonas, and endpoint Tetrahymena cytoplasm (CP) outside of food vacuoles (QD treatment). * Figure 5: High-resolution STEM image and EDS of Tetrahymena that has fed on QD-grown Pseudomonas, after 24 h. , High-angle annular dark-field micrograph of an EDS line scan (large inset) performed through one bright spot (putative CdSe QD as in Fig. 3f) in a region interior to a mitochondrion (small rectangle). , Six EDS spectra acquired in 5 nm steps. Spectra 1, 2 and 6 are external to, 3 and 5 are near the edge of, and 4 is internal to the 'bright spot' (~10 nm across) on the line scan axis (inset). Sloping lines drawn in spectra 2–5 provide baselines for judging peak magnitudes. The spectra clearly show an enrichment of cadmium from the edges to the interior of the bright spot, consistent with a QD-type particle. Note that the Se peak overlaps the Os peak, precluding reliable identification of Se enrichment along this scan. * Figure 6: Mass- and volume-based cadmium concentrations show biomagnification in the predator relative to the prey. ,, Cellular cadmium concentrations with standard error bars for CdSe QD (black bars) and cadmium acetate (white bars) treatments plotted as either cadmium mass per cell volume () or cadmium mass per dry cell biomass (). The concentration ratio of the 16 h Tetrahymena to the 0 h Pseudomonas represents the TTF. Volume- and dry mass-based TTFs were, respectively, 4.82 and 5.37 (QD treatment) and 2.97 and 3.54 (cadmium acetate treatment). Ratios greater than 1 reflect cadmium biomagnification during trophic transfer. Author information * Abstract * Author information * Supplementary information Affiliations * Department of Molecular, Cellular and Developmental Biology, University of California, Santa Barbara, California 93106-9625, USA * R. Werlin & * E. Orias * UC Center for the Environmental Implications of Nanotechnology (UC CEIN), University of California, Santa Barbara, California 93106-5131, USA * R. Werlin, * J. H. Priester, * R. E. Mielke, * S. Jackson, * G. D. Stucky, * G. N. Cherr & * P. A. Holden * Donald Bren School of Environmental Science and Management, University of California, Santa Barbara, California 93106-5131, USA * J. H. Priester, * R. E. Mielke & * P. A. Holden * Earth Research Institute, University of California, Santa Barbara, California 93106-5131, USA * J. H. Priester, * R. E. Mielke & * P. A. Holden * Jet Propulsion Laboratory, California Institute of Technology – NASA, Planetary Science, Pasadena, California 91109-8099, USA * R. E. Mielke * Department of Materials, University of California, Santa Barbara, California 93106-5050, USA * S. Krämer & * G. D. Stucky * Departments of Environmental Toxicology and Nutrition, Bodega Marine Laboratory, University of California, Davis, Bodega Bay, California 94923-0247, USA * S. Jackson & * G. N. Cherr * Department of Chemistry and Biochemistry, University of California, Santa Barbara, California 93106-9510, USA * P. K. Stoimenov & * G. D. Stucky Contributions P.A.H., J.H.P., R.W., E.O. and G.D.S. designed the experiment. P.K.S. and G.D.S. synthesized and provided the quantum dots. R.W. and J.H.P. executed the trophic transfer experiments. R.E.M. and S.K. performed the electron microscopy and EDS analyses. G.N.C. and S.J. determined protein carbonyl content. All authors contributed to the writing of the manuscript. Competing financial interests The authors declare no competing financial interests. Corresponding author Correspondence to: * P. A. Holden Supplementary information * Abstract * Author information * Supplementary information PDF files * Supplementary information (743 KB) Supplementary information Additional data

Friday, January 28, 2011

Hot off the presses! Feb 01 Nat Meth

The Feb 01 issue of the Nat Meth is now up on Pubget (About Nat Meth): if you're at a subscribing institution, just click the link in the latest link at the home page. (Note you'll only be able to get all the PDFs in the issue if your institution subscribes to Pubget.)

Latest Articles Include:

  • The right partner
    - Nat Meth 8(2):97 (2011)
    Nature Methods | Editorial The right partner Journal name:Nature MethodsVolume: 8,Page:97Year published:(2011)DOI:doi:10.1038/nmeth0211-97Published online28 January 2011 For the development, application and dissemination of high-impact methods, interdisciplinary collaboration between experts is vital. View full text Additional data
  • The author file: Hang Lu
    - Nat Meth 8(2):99 (2011)
    Nature Methods | This Month The author file: Hang Lu * Monya Baker Search for this author in: * NPG journals * PubMed * Google ScholarJournal name:Nature MethodsVolume: 8,Page:99Year published:(2011)DOI:doi:10.1038/nmeth0211-99Published online28 January 2011 Practical microsystems are used to monitor flies and worms. View full text Additional data
  • Points of view: Points of review (part 1)
    - Nat Meth 8(2):101 (2011)
    Nature Methods | This Month Points of view: Points of review (part 1) * Bang Wong1 Search for this author in: * NPG journals * PubMed * Google ScholarJournal name:Nature MethodsVolume: 8,Page:101Year published:(2011)DOI:doi:10.1038/nmeth0211-101Published online28 January 2011 Read the full article * Instant access to this article: US$32Buy now * Subscribe to Nature Methods for full access: SubscribeLogin for existing subscribers Additional access options: * Use a document delivery service * Login via Athens * Purchase a site license * Institutional access * British Library Document Supply Centre * Infotrieve * Thompson ISI Document Delivery * You can also request this document from your local library through inter-library loan services. My goal over the next two months is to show concretely how scientific figures can benefit from design principles. I will review concepts from past columns by applying them to several published figures. In the design of common objects, such as a door, when a handle is used many people will mistakenly pull even if the door is to be opened by pushing. When the handle is replaced with a flat plate, which affords pushing, people will know to push. When dealing with figures, we depend on visual cues. We want our figure's layout to express its underlying meaning. View full text Figures at a glance * Figure 1: Layouts can express meaning. () Diagram of a microscopy system. Reprinted from Nature Methods1. () A sketch using grouping and white space to make the three parts of the system being illustrated more apparent. * Figure 2: Visual structure that matches the message. () Illustration showing a gene expression analysis technique. Reprinted from Genome Biology4. () The same elements organized according to the purpose of the illustration, which is to show a sequence of steps. Author information Article tools * Full text * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg Affiliations * Bang Wong is the creative director of the Broad Institute of the Massachusetts Institute of Technology and Harvard and an adjunct assistant professor in the Department of Art as Applied to Medicine at The Johns Hopkins University School of Medicine. Read the full article * Instant access to this article: US$32Buy now * Subscribe to Nature Methods for full access: SubscribeLogin for existing subscribers Additional access options: * Use a document delivery service * Login via Athens * Purchase a site license * Institutional access * British Library Document Supply Centre * Infotrieve * Thompson ISI Document Delivery * You can also request this document from your local library through inter-library loan services. Additional data
  • Resources for proteomics in mouse embryonic stem cells
    - Nat Meth 8(2):103-104 (2011)
    Nature Methods | Correspondence Resources for proteomics in mouse embryonic stem cells * Frank Schnütgen1 Search for this author in: * NPG journals * PubMed * Google Scholar * Franziska Ehrmann1 Search for this author in: * NPG journals * PubMed * Google Scholar * Ina Poser2 Search for this author in: * NPG journals * PubMed * Google Scholar * Nina C Hubner3 Search for this author in: * NPG journals * PubMed * Google Scholar * Jens Hansen4 Search for this author in: * NPG journals * PubMed * Google Scholar * Thomas Floss4 Search for this author in: * NPG journals * PubMed * Google Scholar * Ingrid deVries2 Search for this author in: * NPG journals * PubMed * Google Scholar * Wolfgang Wurst4, 5 Search for this author in: * NPG journals * PubMed * Google Scholar * Anthony Hyman2 Search for this author in: * NPG journals * PubMed * Google Scholar * Matthias Mann3 Search for this author in: * NPG journals * PubMed * Google Scholar * Harald von Melchner1 Contact Harald von Melchner Search for this author in: * NPG journals * PubMed * Google Scholar * Affiliations * Corresponding authorJournal name:Nature MethodsVolume: 8,Pages:103–104Year published:(2011)DOI:doi:10.1038/nmeth0211-103Published online28 January 2011 To the Editor: A recent publication in Nature Methods described recombinase-mediated cassette exchange (RMCE) for re-engineering gene targeted alleles in mouse embryonic stem cells (ESCs) derived from the International Knock Out Mouse Consortium (IKMC) repositories1. We wish to point out that FlipRosaβgeo gene–trapped ESC lines in the same repositories2 can be engineered to encode proteins with N-terminal protein tags using an RMCE-based approach. As do the IKMC's gene-targeted alleles, the FlipRosaβgeo gene-trap alleles include site-specific recombinase target sequences that enable RMCE3 (Fig. 1a). View full text Author information * Author information * Supplementary information Article tools * Full text * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg Affiliations * Department for Molecular Hematology, University of Frankfurt Medical School, Frankfurt am Main, Germany. * Frank Schnütgen, * Franziska Ehrmann & * Harald von Melchner * Max Planck Institute of Molecular Cell Biology and Genetics, Dresden, Germany. * Ina Poser, * Ingrid deVries & * Anthony Hyman * Max Planck Institute of Biochemistry, Martinsried, Germany. * Nina C Hubner & * Matthias Mann * Institute for Developmental Genetics Helmholtz Zentrum München, Germany. * Jens Hansen, * Thomas Floss & * Wolfgang Wurst * German Center for Neurodegenerative Diseases, Technische Universität München, Neuherberg, Germany. * Wolfgang Wurst Competing financial interests The authors declare no competing financial interests. Corresponding author Correspondence to: * Harald von Melchner Supplementary information * Author information * Supplementary information Excel files * Supplementary Table 1 (976K) List of tagging compatible gene trap lines. PDF files * Supplementary Text and Figures (3.1M) Supplementary Figures 1–5, Supplementary Tables 2–3, Supplementary Methods Additional data
  • Data transformation practices in biomedical sciences
    - Nat Meth 8(2):104-105 (2011)
    Nature Methods | Correspondence Data transformation practices in biomedical sciences * Mihai Valcu1, 3 Search for this author in: * NPG journals * PubMed * Google Scholar * Cristina-Maria Valcu2, 3 Contact Cristina-Maria Valcu Search for this author in: * NPG journals * PubMed * Google Scholar * Affiliations * Corresponding authorJournal name:Nature MethodsVolume: 8,Pages:104–105Year published:(2011)DOI:doi:10.1038/nmeth0211-104Published online28 January 2011 To the Editor: In over a century since it was first introduced by William Sealy Gosset (under the pseudonym Student), the t-test has become one of the most common tests in many fields of research1 and is now a basic element in a biologist's toolkit for statistical hypothesis testing. Our screen of the first 2010 issue of medical and biological science journals with an impact factor higher than 15 revealed that in 88 of the 213 research articles, the authors had used t-tests to analyze their data (Supplementary Methods). View full text Author information * Author information * Supplementary information Article tools * Full text * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg Primary authors * These authors contributed equally to this work. * Mihai Valcu & * Cristina-Maria Valcu Affiliations * Department of Behavioral Ecology and Evolutionary Genetics, Max Planck Institute for Ornithology, Seewiesen, Germany. * Mihai Valcu * Department of Experimental and Molecular Pediatric Cardiology, German Heart Centre, Technical University Munich, Munich, Germany. * Cristina-Maria Valcu Competing financial interests The authors declare no competing financial interests. Corresponding author Correspondence to: * Cristina-Maria Valcu Supplementary information * Author information * Supplementary information PDF files * Supplementary Text and Figures (3M) Supplementary Figures 1-3, Supplementary Methods Additional data
  • One genome, two haplotypes
    - Nat Meth 8(2):107 (2011)
    Nature Methods | Research Highlights One genome, two haplotypes * Nicole Rusk Search for this author in: * NPG journals * PubMed * Google ScholarJournal name:Nature MethodsVolume: 8,Page:107Year published:(2011)DOI:doi:10.1038/nmeth0211-107Published online28 January 2011 Two approaches using either fosmid clones or a microfluidic device are used to tackle the challenge of a haplotype-resolved human genome. View full text Subject terms: * Genomics Additional data
  • Rewiring cellular networks
    - Nat Meth 8(2):108-109 (2011)
    Nature Methods | Research Highlights Rewiring cellular networks * Erika Pastrana Search for this author in: * NPG journals * PubMed * Google ScholarJournal name:Nature MethodsVolume: 8,Pages:108–109Year published:(2011)DOI:doi:10.1038/nmeth0211-108aPublished online28 January 2011 RNA-based regulatory systems control the behavior of cells in response to endogenous proteins. View full text Subject terms: * Synthetic Biology Additional data
  • Better living through biochemistry
    - Nat Meth 8(2):108-109 (2011)
    Nature Methods | Research Highlights Better living through biochemistry * Michael Eisenstein Search for this author in: * NPG journals * PubMed * Google ScholarJournal name:Nature MethodsVolume: 8,Pages:108–109Year published:(2011)DOI:doi:10.1038/nmeth0211-108bPublished online28 January 2011 In-depth mass spectrometric analysis reveals how cells survive stress by coordinating various enzymes that modify RNAs involved in protein synthesis. View full text Subject terms: * Biochemistry Additional data
  • News in brief
    - Nat Meth 8(2):109 (2011)
    Nature Methods | Research Highlights News in brief Journal name:Nature MethodsVolume: 8,Page:109Year published:(2011)DOI:doi:10.1038/nmeth0211-109Published online28 January 2011 Read the full article * FREE access with registration Register now * Already have a Nature.com account? Login Additional access options: * Use a document delivery service * Login via Athens * Purchase a site license * Institutional access * British Library Document Supply Centre * Infotrieve * Thompson ISI Document Delivery * You can also request this document from your local library through inter-library loan services. An RNA crystallization chaperone The crystallization of RNA molecules for structural analysis is even more challenging than protein crystallization owing to the low chemical diversity, flexibility and conformational heterogeneity of RNA. Koldobskaya et al. introduce a chaperone system that stabilizes RNA structure and promotes crystallization. The chaperone is an antigen-binding fragment (Fab) that recognizes an epitope tag that can be installed on any RNA of interest. Koldobskaya, Y.et al. Nat. Struct. Mol. Biol.18, 100–106 (2011). View full text Read the full article * FREE access with registration Register now * Already have a Nature.com account? Login Additional access options: * Use a document delivery service * Login via Athens * Purchase a site license * Institutional access * British Library Document Supply Centre * Infotrieve * Thompson ISI Document Delivery * You can also request this document from your local library through inter-library loan services. Additional data
  • Differentiation in three dimensions
    - Nat Meth 8(2):111 (2011)
    Nature Methods | Research Highlights Differentiation in three dimensions * Monya Baker Search for this author in: * NPG journals * PubMed * Google ScholarJournal name:Nature MethodsVolume: 8,Page:111Year published:(2011)DOI:doi:10.1038/nmeth0211-111Published online28 January 2011 Pluripotent stem cells form intestine-like structures in vitro. View full text Subject terms: * Stem Cells Additional data
  • A genetic system to study reprogramming
    - Nat Meth 8(2):112 (2011)
    Nature Methods | Research Highlights A genetic system to study reprogramming * Natalie de Souza Search for this author in: * NPG journals * PubMed * Google ScholarJournal name:Nature MethodsVolume: 8,Page:112Year published:(2011)DOI:doi:10.1038/nmeth0211-112Published online28 January 2011 Caenorhabditis elegans can be used to probe the mechanistic basis for cell-fate conversion. View full text Subject terms: * Genetics Additional data
  • Synthesis through sequencing
    - Nat Meth 8(2):114 (2011)
    Nature Methods | Research Highlights Synthesis through sequencing * Daniel Evanko Search for this author in: * NPG journals * PubMed * Google ScholarJournal name:Nature MethodsVolume: 8,Page:114Year published:(2011)DOI:doi:10.1038/nmeth0211-114Published online28 January 2011 Next-generation sequencing platforms provide both high-throughput sequencing and DNA production. View full text Subject terms: * Synthetic Biology Additional data
  • Metabolomics: from small molecules to big ideas
    - Nat Meth 8(2):117-121 (2011)
    Nature Methods | Technology Feature Metabolomics: from small molecules to big ideas * Monya Baker1 Contact Monya Baker Search for this author in: * NPG journals * PubMed * Google ScholarJournal name:Nature MethodsVolume: 8,Pages:117–121Year published:(2011)DOI:doi:10.1038/nmeth0211-117Published online28 January 2011 The focus of metabolomic studies is shifting from cataloging chemical structures to finding biological stories. View full text Author information Article tools * Full text * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg Affiliations * Monya Baker is technology editor for Nature and Nature Methods Corresponding author Correspondence to: * Monya Baker Additional data
  • Five challenges to bringing single-molecule force spectroscopy into living cells
    - Nat Meth 8(2):123-127 (2011)
    Nature Methods | Commentary Five challenges to bringing single-molecule force spectroscopy into living cells * Yves F Dufrêne1 Search for this author in: * NPG journals * PubMed * Google Scholar * Evan Evans2 Search for this author in: * NPG journals * PubMed * Google Scholar * Andreas Engel3 Search for this author in: * NPG journals * PubMed * Google Scholar * Jonne Helenius4 Search for this author in: * NPG journals * PubMed * Google Scholar * Hermann E Gaub5 Search for this author in: * NPG journals * PubMed * Google Scholar * Daniel J Müller4 Contact Daniel J Müller Search for this author in: * NPG journals * PubMed * Google Scholar * Affiliations * Corresponding authorJournal name:Nature MethodsVolume: 8,Pages:123–127Year published:(2011)DOI:doi:10.1038/nmeth0211-123Published online28 January 2011 In recent years, single-molecule force spectroscopy techniques have been used to study how inter- and intramolecular interactions control the assembly and functional state of biomolecular machinery in vitro. Here we discuss the problems and challenges that need to be addressed to bring these technologies into living cells and to learn how cellular machinery is controlled in vivo. View full text Figures at a glance * Figure 1: SMFS of the cell's molecular machinery. () SMFS methods rely on different force probes to quantify interactions: AFM uses ~10–200-micrometer-long cantilevers5, 13, optical and magnetic tweezers use beads4, pressurized microcapsules use single cells or vesicles and microneedles1, 3. F, force. Scale bar, 20 μm. () Examples of using force probes (gray spheres) to quantify biomolecular interactions of single biomolecules in vitro (top to bottom): protein unfolding and folding, DNA-binding proteins, ligand-receptor bonds and cytoskeletal motor proteins. * Figure 2: Force-probing cellular interactions in vivo. SMFS offers exciting opportunities to sense interactions that drive the molecular machinery of the cell, including the dynamic assembly of supramolecular complexes, transport phenomena, protein folding, unfolding and degradation, membrane-protein insertion and folding, membrane shaping and reorganization, DNA-binding proteins, cell adhesion and signaling, signaling pathways or interactions of the cytoskeleton with membrane proteins. Author information Article tools * Full text * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg Affiliations * Yves F. Dufrêne is at Universite catholique de Louvain, Institute of Condensed Matter and Nanosciences, Louvain-la-Neuve, Belgium. * Evan Evans is at Boston University, Medical Engineering and Physics, Boston Massachusetts, USA. * Andreas Engel is in the Department of Pharmacology, Case Western Reserve University, Cleveland, Ohio, USA and at the Biozentrum, University of Basel, Basel, Switzerland. * Jonne Helenius and Daniel J. Müller are at Eidgenössische Technische Hochschule Zürich, Department of Biosystems Science and Engineering, Basel, Switzerland. * Hermann E. Gaub is at Ludwig Maximillians University, Applied Physics, Munich, Germany. Competing financial interests The authors declare no competing financial interests. Corresponding author Correspondence to: * Daniel J Müller Additional data
  • Unrestrained worms bridled by the light
    - Nat Meth 8(2):129-130 (2011)
    Nature Methods | News and Views Unrestrained worms bridled by the light * André E X Brown1 Search for this author in: * NPG journals * PubMed * Google Scholar * William R Schafer1 Contact William R Schafer Search for this author in: * NPG journals * PubMed * Google Scholar * Affiliations * Corresponding authorJournal name:Nature MethodsVolume: 8,Pages:129–130Year published:(2011)DOI:doi:10.1038/nmeth0211-129Published online28 January 2011 Read the full article * Instant access to this article: US$18Buy now * Subscribe to Nature Methods for full access: SubscribeLogin for existing subscribers Additional access options: * Use a document delivery service * Login via Athens * Purchase a site license * Institutional access * British Library Document Supply Centre * Infotrieve * Thompson ISI Document Delivery * You can also request this document from your local library through inter-library loan services. Two systems allow precise optogenetic stimulation of specific neurons in freely behaving nematodes. View full text Author information Article tools * Full text * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg Affiliations * André E.X. Brown and William R. Schafer are in the Division of Cell Biology, Medical Research Council Laboratory of Molecular Biology, Cambridge, UK. Competing financial interests The authors declare no competing financial interests. Corresponding author Correspondence to: * William R Schafer Read the full article * Instant access to this article: US$18Buy now * Subscribe to Nature Methods for full access: SubscribeLogin for existing subscribers Additional access options: * Use a document delivery service * Login via Athens * Purchase a site license * Institutional access * British Library Document Supply Centre * Infotrieve * Thompson ISI Document Delivery * You can also request this document from your local library through inter-library loan services. Additional data
  • New approaches to modeling complex biochemistry
    - Nat Meth 8(2):130-131 (2011)
    Nature Methods | News and Views New approaches to modeling complex biochemistry * John A Bachman1 Search for this author in: * NPG journals * PubMed * Google Scholar * Peter Sorger1 Search for this author in: * NPG journals * PubMed * Google Scholar * AffiliationsJournal name:Nature MethodsVolume: 8,Pages:130–131Year published:(2011)DOI:doi:10.1038/nmeth0211-130Published online28 January 2011 Read the full article * Instant access to this article: US$18Buy now * Subscribe to Nature Methods for full access: SubscribeLogin for existing subscribers Additional access options: * Use a document delivery service * Login via Athens * Purchase a site license * Institutional access * British Library Document Supply Centre * Infotrieve * Thompson ISI Document Delivery * You can also request this document from your local library through inter-library loan services. Combining rule-based descriptions of biochemical reactions with agent-based computer simulation opens new avenues for exploring complex cellular processes. View full text Author information Article tools * Full text * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg Affiliations * John A. Bachman and Peter Sorger are in the Department of Systems Biology, Harvard Medical School, Boston, Massachusetts, USA. Competing financial interests The authors declare no competing financial interests. Read the full article * Instant access to this article: US$18Buy now * Subscribe to Nature Methods for full access: SubscribeLogin for existing subscribers Additional access options: * Use a document delivery service * Login via Athens * Purchase a site license * Institutional access * British Library Document Supply Centre * Infotrieve * Thompson ISI Document Delivery * You can also request this document from your local library through inter-library loan services. Additional data
  • A new way to look at fat
    - Nat Meth 8(2):132-133 (2011)
    Nature Methods | News and Views A new way to look at fat * Joerg Bewersdorf1 Search for this author in: * NPG journals * PubMed * Google Scholar * Robert V Farese Jr2 Search for this author in: * NPG journals * PubMed * Google Scholar * Tobias C Walther1 Contact Tobias C Walther Search for this author in: * NPG journals * PubMed * Google Scholar * Affiliations * Corresponding authorJournal name:Nature MethodsVolume: 8,Pages:132–133Year published:(2011)DOI:doi:10.1038/nmeth0211-132Published online28 January 2011 Read the full article * Instant access to this article: US$18Buy now * Subscribe to Nature Methods for full access: SubscribeLogin for existing subscribers Additional access options: * Use a document delivery service * Login via Athens * Purchase a site license * Institutional access * British Library Document Supply Centre * Infotrieve * Thompson ISI Document Delivery * You can also request this document from your local library through inter-library loan services. Stimulated Raman scattering (SRS) microscopy is used to directly visualize lipids in cells and model organisms, and facilitates screening for genes involved in fat storage. View full text Author information Article tools * Full text * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg Affiliations * Joerg Bewersdorf and Tobias C. Walther are at the Yale University School of Medicine, Department of Cell Biology, New Haven, Connecticut, USA. * Robert V. Farese Jr. is at the J. David Gladstone Institute of Cardiovascular Disease and the Department of Medicine and Department of Biochemistry and Biophysics, University of California San Francisco, San Francisco, California, USA. Competing financial interests J.B. has financial interest in Vutara, a company that produces fluorescence microscopes. Corresponding author Correspondence to: * Tobias C Walther Read the full article * Instant access to this article: US$18Buy now * Subscribe to Nature Methods for full access: SubscribeLogin for existing subscribers Additional access options: * Use a document delivery service * Login via Athens * Purchase a site license * Institutional access * British Library Document Supply Centre * Infotrieve * Thompson ISI Document Delivery * You can also request this document from your local library through inter-library loan services. Additional data
  • RNAi screening for fat regulatory genes with SRS microscopy
    - Nat Meth 8(2):135-138 (2011)
    Nature Methods | Brief Communication RNAi screening for fat regulatory genes with SRS microscopy * Meng C Wang1, 2, 6 Contact Meng C Wang Search for this author in: * NPG journals * PubMed * Google Scholar * Wei Min3, 5, 6 Contact Wei Min Search for this author in: * NPG journals * PubMed * Google Scholar * Christian W Freudiger3, 4 Search for this author in: * NPG journals * PubMed * Google Scholar * Gary Ruvkun2 Search for this author in: * NPG journals * PubMed * Google Scholar * X Sunney Xie3 Contact X Sunney Xie Search for this author in: * NPG journals * PubMed * Google Scholar * Affiliations * Contributions * Corresponding authorsJournal name:Nature MethodsVolume: 8,Pages:135–138Year published:(2011)DOI:doi:10.1038/nmeth.1556Received22 September 2010Accepted17 December 2010Published online16 January 2011 Article tools * Full text * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg Identification of genes regulating fat accumulation is important for basic and medical research; genetic screening for those genes in Caenorhabditis elegans, a widely used model organism, requires in vivo quantification of lipids. We demonstrated RNA interference screening based on quantitative imaging of lipids with label-free stimulated Raman scattering (SRS) microscopy, which overcomes major limitations of coherent anti-Stokes Raman scattering microscopy. Our screening yielded eight new genetic regulators of fat storage. View full text Figures at a glance * Figure 1: Visualization of cellular fat storage in lipid droplets using SRS microscopy. () Experimental scheme of label-free SRS microscopy for in vivo lipid imaging. PMT, photomultipier tube. (–) YFP fluorescence images (–), SRS signals (–) and merged images (–) of HEK 293 cells expressing YFP-tagged perilipin A (,,), ADFP (,,) and LSDP5 (,,). Scale bars, 1 μm. * Figure 2: Imaging fat accumulation and distribution in C. elegans by SRS microscopy. (,) SRS signals revealed fat storage in intestine (arrow), hypodermis (asterisk), early embryos in the uterus (arrowhead) and cellular nuclei (labeled with "n"). () Subcelluar fat accumulation in a pool of droplets observed by SRS microscopy. (–) Two-photon–excited fluorescence from Nile Red staining (), SRS signals () and the overlaid images of these two signals (). (–) BODIPY staining of two distinct groups of subcellular organelles with weaker (asterisk) and stronger (arrow) fluorescence signals (), (SRS) image of the same organelles (), and overlap of BODIPY and SARS signals (). (,) CARS images showing strong signals in the intestinal cell nuclei owing to nonresonant background () and SRS image of the same worm with dark nuclei in the intestinal cells (). (–) CARS and SRS images of the same worm taken at a Raman shift of 2,845 cm−1 resonant with CH2 stretching mode (,) and a Raman shift of 2,796 cm−1 off-resonant (,). Cross-section profiles of the regions! marked by gray lines in and are shown in . Scale bars, 50 μm. * Figure 3: RNAi screening of new fat storage regulatory genes based on in vivo lipid quantification using label-free SRS microscopy. (–) Fat was visualized by SRS in the wild-type worm (), the daf-2(e1370) mutant () and the transgenic worm intestinally overexpressing the K04A8.5 lipase () under same imaging conditions. () Quantification of fat content by SRS (n = 5 worms) and thin-layer chromatography–gas chromatography (TLC/GC) (n = 5 × 103 worms). () SRS signal increase compared to the control for genes that resulted in a fat content increase of more than 25% when inactivated by RNAi (P < 0.0001, n = 5 worms). Control, worms fed with bacteria containing empty vectors. All the experiments were performed twice independently. Results from one experiment are shown. () Normal fat accumulation as observed in the RNAi hypersensitive strain, nre-1(hd20)lin-15b(hd126), fed with empty vector–containing bacteria (control). (–) SRS images of three candidate worms. Scale bars, 50 μm. Error bars, s.d. Author information * Author information * Supplementary information Primary authors * These authors contributed equally to this work. * Meng C Wang & * Wei Min Affiliations * Department of Molecular and Human Genetics and Huffington Center on Aging, Baylor College of Medicine, Houston, Texas, USA. * Meng C Wang * Department of Molecular Biology, Massachusetts General Hospital, and Department of Genetics, Harvard Medical School, Boston, Massachusetts, USA. * Meng C Wang & * Gary Ruvkun * Department of Chemistry and Chemical Biology, Harvard University, Cambridge, Massachusetts, USA. * Wei Min, * Christian W Freudiger & * X Sunney Xie * Department of Physics, Harvard University, Cambridge, Massachusetts, USA. * Christian W Freudiger * Present address: Department of Chemistry, Columbia University, New York, New York, USA. * Wei Min Contributions M.C.W., W.M. and X.S.X. conceived the study; M.C.W. and W.M. designed the experiments; M.C.W., W.M. and C.W.F. performed the experiments; M.C.W. analyzed the data; M.C.W., W.M., G.R. and X.S.X. wrote the manuscript. Competing financial interests The authors declare no competing financial interests. Corresponding authors Correspondence to: * X Sunney Xie or * Meng C Wang or * Wei Min Supplementary information * Author information * Supplementary information PDF files * Supplementary Text and Figures (2M) Supplementary Figures 1– 4 and Supplementary Table 1 Additional data
  • Simultaneous two-photon calcium imaging at different depths with spatiotemporal multiplexing
    - Nat Meth 8(2):139-142 (2011)
    Nature Methods | Brief Communication Simultaneous two-photon calcium imaging at different depths with spatiotemporal multiplexing * Adrian Cheng1, 2, 3, 5 Search for this author in: * NPG journals * PubMed * Google Scholar * J Tiago Gonçalves2, 5 Search for this author in: * NPG journals * PubMed * Google Scholar * Peyman Golshani2 Search for this author in: * NPG journals * PubMed * Google Scholar * Katsushi Arisaka1, 4 Search for this author in: * NPG journals * PubMed * Google Scholar * Carlos Portera-Cailliau2, 3 Contact Carlos Portera-Cailliau Search for this author in: * NPG journals * PubMed * Google Scholar * Affiliations * Contributions * Corresponding authorJournal name:Nature MethodsVolume: 8,Pages:139–142Year published:(2011)DOI:doi:10.1038/nmeth.1552Received01 October 2010Accepted14 December 2010Published online09 January 2011 Article tools * Full text * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg In vivo two-photon calcium imaging would benefit from the use of multiple excitation beams to increase scanning speed, signal-to-noise ratio and field of view or to image different axial planes simultaneously. Using spatiotemporal multiplexing we circumvented light-scattering ambiguity inherent to deep-tissue multifocal two-photon microscopy. We demonstrate calcium imaging at multiple axial planes in the intact mouse brain to monitor network activity of ensembles of cortical neurons in three spatial dimensions. View full text Figures at a glance * Figure 1: Spatiotemporal multiplexing to overcome depth limitations in multifocal 2PLSM. () Layout of the prototype microscope. Laser pulses are emitted with a 12-ns period from a commercial ultrafast Ti:Al203 laser. The beam is divided into four beams, which are delayed by 3 ns each (1 m per 3 ns) and converged on the slow-axis scan mirror aperture, which is then projected onto the objective back aperture. The resulting emitted fluorescence, which is highly scattered, is collected by two hybrid photodetectors. The hybrid photodetector's active area is placed in a demagnified conjugate plane of the objective back aperture to maximize scattered light collection. () Schematic of different beam-scanning patterns at the sample. Time multiplexing removes ambiguity between different imaging planes, allowing both axial and lateral beam distribution. () Time course of detected fluorescence signal for a single beam (top) and four spatiotemporally multiplexed beams (bottom). Overlay of 200 oscilloscope traces and summary histograms of single photoelectron events (using a ! pollen grain). Fluorescence from different time windows (different colors) is associated with different delayed excitation beams. Scale bar, 12 ns. * Figure 2: Multifocal two- and three-dimension in vivo 2PCI of L2/3 neurons in barrel cortex with spatiotemporal multiplexing. () Spatial distribution of four beams in a single image plane (left) and typical field of view (right), an average intensity time projection of a representative calcium imaging movie (3 min, 250 frames s−1) from a P20 mouse using Fluo-4 AM. Scale bar, 50 μm. () Zero-lag cross-correlation image computed from a movie. () Final segmented image of cell bodies obtained through morphological filters (red contours). () Raw calcium traces of 11 different cells (neurophil signal in blue). () Model calcium traces with identified neuronal spiking events (tic marks) of selected cells using a peeling algorithm are shown with relative fluorescence change (ΔF/F). (,) Details of shaded regions shown in and , respectively. () Spatial distribution of four beams arranged axially (left) and field of view for each imaging plane (right). Images are average intensity time projections of a typical movie with Fluo-4 AM (3 min, 60 volumes s−1) with depth spanning from 90 μm to 180 μm below th! e pia (encompassing layers 1 to 3). Scale bar, 50 μm. () Zero-lag cross-correlation image (left) and fully segmented image (right) with cell contours (red). () Selected traces reconstructed by the peeling algorithm, with rows in and corresponding to beams shown in . * Figure 3: Multifocal 2PCI with spatiotemporal multiplexing to assess activity-derived neuronal connectivity in L2/3 of barrel cortex. () Spatial distribution of four scanning beams (left) and representative field of view in two separate imaging planes (right) from an experiment with a P20 mouse using Fluo-4 AM (3 min, 100 frames s−1). Scale bar, 50 μm. () Zero-lag cross-correlation image (left) and segmented image (right) of the same experiment, with rows in corresponding to rows in . Cells are numerically ordered according to their vertical coordinates. () Raster plot showing identified spiking events in cells from . Events shown in red were identified as having participated in a peak of synchrony (bottom trace). () Peak correlation coefficient (over a time lag of ± 1 s) for significantly correlated (P < 0.05; as defined in Online Methods) cells shown in . () Axial (depth) versus radial (lateral) spread of bursts of neuronal firing corresponding to peaks of synchrony identified in several movies (10 movies from 2 mice, 173 peaks of synchrony). A minority of bursts had a spatial organization consistent! with either columnar (top left) or laminar connectivity (bottom right). () Peak correlation coefficients from versus cell pair radial distance (ΔR), for cell pairs in different imaging planes, the same imaging plane and for all pairs (10 movies, 10,262 pairs). Error bars, s.e.m. Author information * Author information * Supplementary information Primary authors * These authors contributed equally to this work. * Adrian Cheng & * J Tiago Gonçalves Affiliations * Department of Physics and Astronomy, University of California Los Angeles, Los Angeles, California, USA. * Adrian Cheng & * Katsushi Arisaka * Department of Neurology, David Geffen School of Medicine, University of California Los Angeles, Los Angeles, California, USA. * Adrian Cheng, * J Tiago Gonçalves, * Peyman Golshani & * Carlos Portera-Cailliau * Department of Neurobiology, David Geffen School of Medicine, University of California Los Angeles, Los Angeles, California, USA. * Adrian Cheng & * Carlos Portera-Cailliau * California NanoSystems Institute,University of California, Los Angeles, Los Angeles, California, USA. * Katsushi Arisaka Contributions A.C., J.T.G., P.G., K.A. and C.P.-C. conceived the project. A.C. designed and built the microscope and control electronics, and developed the microscope software. J.T.G. performed in vivo multifocal calcium imaging and simultaneous cell-attached recordings. A.C. analyzed the data. A.C., J.T.G. and C.P.-C. wrote the manuscript. K.A. and C.P.-C. supervised the project. Competing financial interests The authors declare no competing financial interests. Corresponding author Correspondence to: * Carlos Portera-Cailliau Supplementary information * Author information * Supplementary information PDF files * Supplementary Text and Figures (6M) Supplementary Figures 1–8 and Supplementary Note 1 Additional data
  • A photoprotection strategy for microsecond-resolution single-molecule fluorescence spectroscopy
    - Nat Meth 8(2):143-146 (2011)
    Nature Methods | Brief Communication A photoprotection strategy for microsecond-resolution single-molecule fluorescence spectroscopy * Luis A Campos1, 2, 4 Search for this author in: * NPG journals * PubMed * Google Scholar * Jianwei Liu2, 3, 4 Search for this author in: * NPG journals * PubMed * Google Scholar * Xiang Wang2, 3 Search for this author in: * NPG journals * PubMed * Google Scholar * Ravishankar Ramanathan1 Search for this author in: * NPG journals * PubMed * Google Scholar * Douglas S English2, 3 Search for this author in: * NPG journals * PubMed * Google Scholar * Victor Muñoz1, 2 Contact Victor Muñoz Search for this author in: * NPG journals * PubMed * Google Scholar * Affiliations * Contributions * Corresponding authorJournal name:Nature MethodsVolume: 8,Pages:143–146Year published:(2011)DOI:doi:10.1038/nmeth.1553Received27 April 2010Accepted07 December 2010Published online09 January 2011 Article tools * Full text * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg Time resolution of current single-molecule fluorescence techniques is limited to milliseconds because of dye blinking and bleaching. Here we introduce a photoprotection strategy that affords microsecond resolution by combining efficient triplet quenching by oxygen and Trolox with minimized bleaching via the oxygen radical scavenger cysteamine. Using this approach we resolved the single-molecule microsecond conformational fluctuations of two proteins: the two-state folder α-spectrin SH3 domain and the ultrafast downhill folder BBL. View full text Figures at a glance * Figure 1: Effect of photoprotectors on the photon throughput of B-DNA10 labeled with A488-A594 at 10-base-pair separation. () We irradiated the DNA with high continuous wave 485-nm laser excitation intensities and collected 100-μs bins with more than 50 total photons (donor plus acceptor) over the background, which we termed high-emission bursts for simplicity. Plotted are the high-emission bursts detected in one minute from free diffusing single molecules. The lines are fits to polynomial functions. Trolox-cysteamine, 1 mM Trolox and 10 mM cysteamine. (–) FRET efficiency histograms calculated from the high-emission bursts collected over a 5-min period with irradiance of 525 kW cm−2. Asterisk, bulk FRET efficiency. () High-emission bursts min−1 at 700 kW cm−2 irradiance for indicated combinations of photoprotectors. Error bars, s.d. (five experiments). OS, enzymatic oxygen scavenger as described in reference 6 and Online Methods. * Figure 2: Microsecond-resolution free-diffusion single-molecule FRET experiments of α-spectrin SH3 domain labeled with A488-A594 on two cysteines introduced at the protein ends. () Examples of FRET efficiency trajectories of α-spectrin SH3 domain single molecules freely diffusing through the observation volume of the confocal microscope. The time resolution was 50 μs, and colors represent the number of photons (n) in each 50-μs bin. Shown are examples of trajectories of folded molecules (~35% of the total; top row); trajectories of unfolded molecules (~40% of the total; second row); trajectories with the acceptor in a dark state (12% of the total; third row); and trajectories that showed bleaching or long-lasting blinking (bottom row). () FRET-efficiency histograms at indicated urea concentrations obtained from 1-ms bins with >200 photons (left) and from 100-μs bins of >50 photons after pruning all single-molecule diffusive trajectories that visited the (dark-acceptor state) (FRET efficiency values below 0.2) at any point (right). () Free energy of unfolding as a function of urea concentration calculated from the relative areas of the folded (~0! .75 FRET efficiency) and unfolded (~0.4 FRET efficiency) peaks compared to the bulk estimate (dark blue line). The red line shows the linear regression to the single-molecule data obtained with 1-ms binning for reference. () Comparison of the two FRET-efficiency histograms at 2 M urea expanded to highlight the artifacts in the intermediate FRET-efficiency region. * Figure 3: Microsecond resolution free diffusion single-molecule FRET of BBL. () A three-dimensional structure of BBL labeled with A488 (cyan) and A594 (red) on the ends of long unstructured tails. () FRET efficiency histograms of labeled BBL in 5 M urea (the denaturation midpoint (Cm) was ~5.3 M) obtained from 50-μs bins (left) and 1-ms bins (right) with > 40 total photons over background. The expected shot-noise width is shown in red and the FRET efficiency value at the Cm is indicated with a black vertical line. () FRET-efficiency autocorrelation function (R) calculated from experimental free diffusion trajectories (blue) and from the maximum likelihood fit to a seven-states model (green). The red curves are fits to an exponential function with the indicated relaxation times. () Examples of free-diffusing BBL trajectories near the denaturation midpoint (cyan circles). The red lines show the fit to the seven-states model for each trajectory. () Cartoon of the stochastic dynamic simulations on a harmonic potential. () FRET-efficiency autocorrelation! function (R) for the downhill simulation. The fit (red curve) to a single exponential function is shown with the relaxation time indicated. () A 10-ms single-molecule trajectory simulated with the stochastic downhill model sketched in . A simulation of shot-noise corresponding to a 0.8 MHz photon count rate (dark blue) and the fit to the seven-states model (red). Author information * Author information * Supplementary information Primary authors * These authors contributed equally to this work. * Luis A Campos & * Jianwei Liu Affiliations * Centro de Investigaciones Biológicas, Consejo Superior de Investigaciones Científicas, Madrid, Spain. * Luis A Campos, * Ravishankar Ramanathan & * Victor Muñoz * Department of Chemistry and Biochemistry, University of Maryland, College Park, Maryland, USA. * Luis A Campos, * Jianwei Liu, * Xiang Wang, * Douglas S English & * Victor Muñoz * Present addresses: Department of Pediatrics, Stanford University, Stanford, California, USA (J.L.), Department of Chemistry, University of North Carolina, Chapel Hill, North Carolina, USA (X.W.) and Department of Chemistry, Wichita State University, Wichita, Kansas, USA (D.S.E.). * Jianwei Liu, * Xiang Wang & * Douglas S English Contributions L.A.C. and J.L. prepared samples, identified the oxygen radical scavengers, performed experiments and analyzed data. L.A.C. performed all the additional experiments requested by the reviewers. X.W. acquired and analyzed data. R.R. performed the stochastic simulations of downhill folding. D.S.E. supervised data acquisition and designed research. V.M. designed research, supervised data acquisition, performed and supervised data analysis and simulations, and wrote the manuscript. Competing financial interests The authors declare no competing financial interests. Corresponding author Correspondence to: * Victor Muñoz Supplementary information * Author information * Supplementary information PDF files * Supplementary Text and Figures (524K) Supplementary Figures 1–4 and Supplementary Table 1 Additional data
  • Optogenetic manipulation of neural activity in freely moving Caenorhabditis elegans
    - Nat Meth 8(2):147-152 (2011)
    Nature Methods | Article Optogenetic manipulation of neural activity in freely moving Caenorhabditis elegans * Andrew M Leifer1, 4 Search for this author in: * NPG journals * PubMed * Google Scholar * Christopher Fang-Yen1, 2, 4 Contact Christopher Fang-Yen Search for this author in: * NPG journals * PubMed * Google Scholar * Marc Gershow1 Search for this author in: * NPG journals * PubMed * Google Scholar * Mark J Alkema3 Search for this author in: * NPG journals * PubMed * Google Scholar * Aravinthan D T Samuel1 Contact Aravinthan D T Samuel Search for this author in: * NPG journals * PubMed * Google Scholar * Affiliations * Contributions * Corresponding authorsJournal name:Nature MethodsVolume: 8,Pages:147–152Year published:(2011)DOI:doi:10.1038/nmeth.1554Received23 August 2010Accepted16 December 2010Published online16 January 2011 Abstract * Abstract * Author information * Supplementary information Article tools * Full text * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg We present an optogenetic illumination system capable of real-time light delivery with high spatial resolution to specified targets in freely moving Caenorhabditis elegans. A tracking microscope records the motion of an unrestrained worm expressing channelrhodopsin-2 or halorhodopsin in specific cell types. Image processing software analyzes the worm's position in each video frame, rapidly estimates the locations of targeted cells and instructs a digital micromirror device to illuminate targeted cells with laser light of the appropriate wavelengths to stimulate or inhibit activity. Because each cell in an unrestrained worm is a rapidly moving target, our system operates at high speed (~50 frames per second) to provide high spatial resolution (~30 μm). To test the accuracy, flexibility and utility of our system, we performed optogenetic analyses of the worm motor circuit, egg-laying circuit and mechanosensory circuits that have not been possible with previous methods. View full text Figures at a glance * Figure 1: High-resolution optogenetic control of freely moving C. elegans. () An individual worm swims or crawls on a motorized stage under red dark-field illumination. A high-speed camera images the worm. Custom software instructs a DMD to reflect laser light onto targeted cells. () Images are acquired and processed at ~50 FPS. Each 1,024 × 768 pixel image is thresholded and the worm boundary is found. Head and tail are located as maxima of boundary curvature (red arrows). Centerline is calculated from the midpoint of line segments connecting dorsal and ventral boundaries (blue bar) and is resampled to contain 100 equally spaced points. The worm is partitioned into segments by finding vectors (green arrows) from centerline to boundary, and selecting one that is most perpendicular to the centerline (orange arrow). Targets defined in worm coordinates are transformed into image coordinates and sent to the DMD for illumination (green bar). () Schematic of body-wall muscles. Anterior, to left; dorsal, to top. Bending wave speed of swimming worm expres! sing Halo/NpHR in its body-wall muscles subjected to green light (10 mW mm−2) outside or inside the worm boundary (n = 5 worms, representative trace). () Schematic of HSN. A swimming worm expressing ChR2 in HSN was subjected to blue light (5 mW mm−2). Histogram, position at which egg-laying occurred when a narrow stripe of light was slowly scanned along the worm's centerline (n = 13 worms). Once an egg was laid, the worm was discarded. * Figure 2: Optogenetic inactivation of muscle cells. () Kymograph of time-varying body curvature along the centerline of a Pmyo3Halo/NpHRCFP transgenic worm. Between 0 s and 4 s, the worm was stimulated with green light (10 mW mm−2) in a region spanning the worm diameter and between 0.38 and 0.6 of the fractional distance along the centerline. () For the kymograph in , time-varying curvature at two points along the worm centerline, both anterior (top) and posterior (bottom) to the illuminated region. * Figure 3: Inhibition of motor neurons. () Schematic of cholinergic DB and VB motor neurons. Anterior, to left; dorsal, to top. Kymograph of time-varying body curvature along the centerline of a Punc-17Halo/NpHRCFP transgenic worm illuminated by a stripe of green light (10 mW mm−2) along its VNC between t = 0 s and 1.6 s. In the dorsal-ventral direction, the stripe width was equal to 50% of the worm diameter and centered on the ventral boundary. In the anterior-posterior direction, the stripe length was between 0.14 and 0.28 of the fractional distance along the body. () For the kymograph in , time-varying curvature at two points along the worm centerline, both anterior (top) and posterior (bottom) to the illuminated region. () Video sequence of worm illuminated by a long stripe of green light (10 mW mm−2) spanning the VNC between t = 0 s and 1.8 s. Scale bar, ~100 μm. () Bending wave speed of a swimming worm illuminated by a long stripe of green light (10 mW mm−2) lasting 1.8 s and spanning the VNC (top) an! d dorsal nerve cord (bottom). * Figure 4: Optogenetic analysis of mechanosensory neurons. () Top, schematic of anterior and posterior touch receptor cells. Anterior, to left; dorsal, to top. Kymographs (left) of time-varying curvature of centerline of worms expressing ChR2 in mechanosensory neurons (Pmec-4ChR2GFP) subjected to rectangles of blue light (5 mW mm−2) targeting different groups of touch receptor neurons. Plots of bending wave speed (right) indicate stimulus-evoked changes in direction or speed. AVM and ALM neurons are subjected to 1.5 s of stimulation. Given a coordinate system where x specifies dorsal-ventral location (–1, dorsal boundary; 0, centerline; 1, ventral boundary) and y defines fractional distance along the worm's centerline (0, head; 1, tail), the rectangle of illumination has corners (x,y) = ((–1.1,0),(1.1,0.46)). () PVM and PLM neurons are subjected to 2.5 s of stimulation with a rectangular illumination (n = 5 worms, representative trace) with corners at (x,y) = ((–1.1,0.62),(1.1,0.99)). () ALM cell body is specifically stimula! ted by illuminating a small rectangle with corners at (x,y) = ((–0.3,0.38), (–0.9,0.46)). () AVM cell body is specifically stimulated by illuminating a small rectangle with corners at (x,y) = ((0.3,0.3),(0.9,0.38)). * Figure 5: Habituation of individual touch receptor neuronal types. (,) Schematic showing anterior and posterior touch receptor neurons (top). Anterior, to left; dorsal, to top. A freely swimming worm expressing Kaede in touch receptor neurons was continuously tracked and illuminated with a small rectangle of 405-nm light (2 mW mm−2) centered on either AVM or ALM (as in Fig. 4c,d) for 60 s. Red and green fluorescence images are shown. Scale bars, 100 μm. () Individual ALM and AVM neurons were repeatedly stimulated with blue light (5 mW mm−2) for 1.5 s every 60 s for ~40 min, either alone () or interleaved within each experiment (; ALM, 30 s; AVM, 30 s; ALM, 30 s; and so on). Fractional response to stimulus of each neuronal type was fit to an exponential, a + b exp(–t/τ), using maximum likelihood estimator. Time constant for habituation, τ, was extracted from each fit. Error bars, s.e.m. Fractional response of ALM when stimulated alone (; n = 7 worms). Fractional response of AVM when stimulated alone (; n = 8 worms). Fractional respo! nse of ALM (left) and AVM (right) during interleaved stimulation of both (; n = 7 worms). Author information * Abstract * Author information * Supplementary information Primary authors * These authors contributed equally to this work. * Andrew M Leifer & * Christopher Fang-Yen Affiliations * Department of Physics and Center for Brain Science, Harvard University, Cambridge, Massachusetts, USA. * Andrew M Leifer, * Christopher Fang-Yen, * Marc Gershow & * Aravinthan D T Samuel * Department of Bioengineering, University of Pennsylvania, Philadelphia, Pennsylvania, USA. * Christopher Fang-Yen * Department of Neurobiology, University of Massachusetts Medical School, Worcester, Massachusetts, USA. * Mark J Alkema Contributions C.F.-Y. and A.M.L. designed the hardware setup; A.M.L. wrote the software, with supervision from M.G.; A.M.L., C.F.-Y., M.J.A. and A.D.T.S. designed experiments; A.M.L. carried out experiments; A.M.L. and C.F.-Y. analyzed data with advice from M.G.; A.M.L., C.F.-Y. and A.D.T.S. wrote the manuscript. Competing financial interests The authors declare no competing financial interests. Corresponding authors Correspondence to: * Christopher Fang-Yen or * Aravinthan D T Samuel Supplementary information * Abstract * Author information * Supplementary information Movies * Supplementary Video 1 (5M) A Pmyo-3::Halo::CFP worm expressing Halorhodopsin in muscle is induced to relax only when the Colbert system illuminates within the worm's body. The movie shows the same individual as shown in Figure 1c. During frames 6707–6771, the entire region outside the worm's boundary is illuminated with green light (10 mW mm−2) and the worm continues locomotion. During frames 6,847–6,917, only the region inside the boundary of the worm is illuminated and the worm relaxes. During frames 7,052–7,117 only the region outside the worm's boundary is illuminated and the worm continues moving normally. The frame number is indicated at the bottom right. Light green shading indicates the area where the system is targeting. Bright green shading and the appearance of the words "DLP ON" indicate that the system is illuminating the targeted area. * Supplementary Video 2 (8M) An Pegl-6::ChR2::GFP worm is induced to lay eggs when a stripe of blue light reaches HSN. The video shows the same individual as in Figure 1d. A narrow stripe of light (5 mW mm−2), 0.02 of the fractional length along the worm centerline and twice the width of the worm, progresses from the worm's head towards its tail. The stripe takes steps of 0.02 fractional worm lengths and illuminates for 4 s at each step. At frame 8,828, the illumination band reaches HSN and the worm lays eggs. The frame number is indicated at the bottom right. * Supplementary Video 3 (960K) The bending waves of a Pmyo-3::Halo::CFP transgenic worm are dampened and the anterior relaxes when a portion of the worm is illuminated with green light. The video shows the same individual as in Figure 2. The illumination is turned on 4 s into the movie. The worm recovers after the illumination is turned off. Light grey shading indicates the area where the system is targeting. . Light green shading indicates the area where the system is targeting. Bright green shading and the appearance of the words "DLP ON" indicate that the system is illuminating the target. * Supplementary Video 4 (3M) The bending waves of an Punc-17::Halo::CFP are abolished when a small ventral region near the worm's head is illuminated. The video shows the same individual as shown in Figure 3a,b. During frames 9,075 to 9,141, the worm is illuminated with green light (10 mW mm−2) and no bending waves are propagated from the head to the tail. On the contrary, the worm is paralyzed posterior to the region of illumination and its curvature is frozen. Only after the stimulation ends, are bending waves again able to propagate from the anterior to posterior of the worm. The frame number is indicated at the bottom right. Light green shading indicates the area where the system is targeting. Bright green shading and the appearance of the words "DLP ON" indicate that the system is illuminating the target. * Supplementary Video 5 (8M) An Punc-17::Halo::CFP transgenic worm is paralyzed only when the ventral nerve cord is illuminated, but not when the dorsal nerve cord is illuminated. The video shows the same 988kindividual as in Figure 3c,d. The ventral nerve cord is illuminated with green light at 10 mW mm−2 (frames 37,909–37,971) and then the the dorsal nerve cord is illuminated (frames 38,233–38,295). Note that during paralysis the worm does not relax to a neutral position. Light green shading indicates the area where the system is targeting. Bright green shading and the appearance of the words "DLP ON" indicate that the system is illuminating the target. * Supplementary Video 6 (988K) The anterior of a Pmec-4::ChR2::GFP worm is illuminated for 1.5s, inducing a reversal. The video shows the same individual as in Figure 4a. During frames 7,645–7,709, the anterior 46% of the worm is illuminated with blue light at 5 mW mm−2, which includes the neurons AVM and ALM and their associated processes. The frame number is indicated in the bottom right hand corner. Light blue shading indicates the area where the system is targeting. Bright blue shading and the appearance of the words "DLP ON" indicate that the system is illuminating the target. * Supplementary Video 7 (2M) The posterior of a Pmec-4::ChR2::GFP worm is illuminated with blue light, inducing forward movement. The video shows the same individual as in Figure 4b. During frames 13,655–13,733, the posterior 38% of the worm, which includes the neurons PVM and PLM and their associated processes is illuminated with blue light (5 mW mm−2) for 1.5 s. The worm, originally in a resting state, moves forward. The frame number is indicated in the bottom right hand corner. Light blue shading indicates the area where the system is targeting. Bright blue shading and the appearance of the words "DLP ON" indicate that the system is illuminating the target. * Supplementary Video 8 (2M) The cell bodies of ALM in a Pmec-4::ChR2::GFP worm are illuminated with blue light, inducing a reversal. The video shows the same individual as in Figure 4c. During frames 2,013−2,079, ALM is illuminated with blue light (5 mW mm−2) for 1.5 s. The worm subsequently reverses. The frame number is indicated in the bottom right hand corner. Light blue shading indicates the area where the system is targeting. Bright blue shading and the appearance of the words "DLP ON" indicate that the system is illuminating the target. * Supplementary Video 9 (896K) The cell body of the single neuron AVM in a Pmec-4::ChR2::GFP is illuminated with blue light, initiating a reversal. The video shows the same individual as in Figure 4d. During frames 1,925–1,994, AVM is illuminated with blue light (5 mW mm−2) for 1.5 and the worm subsequently undergoes a reversal. The frame number is indicated in the bottom right hand corner. Light blue shading indicates the area where the system is targeting. Bright blue shading and the appearance of the words "DLP ON" indicate that the system is illuminating the target. Zip files * Supplementary Software (2M) MindControl is software, written in the C programming language, used to track a worm and create illumination patterns in real time. Documentation is also included. Additional data
  • Real-time multimodal optical control of neurons and muscles in freely behaving Caenorhabditis elegans
    - Nat Meth 8(2):153-158 (2011)
    Nature Methods | Article Real-time multimodal optical control of neurons and muscles in freely behaving Caenorhabditis elegans * Jeffrey N Stirman1, 2 Search for this author in: * NPG journals * PubMed * Google Scholar * Matthew M Crane2 Search for this author in: * NPG journals * PubMed * Google Scholar * Steven J Husson3, 4 Search for this author in: * NPG journals * PubMed * Google Scholar * Sebastian Wabnig3, 4 Search for this author in: * NPG journals * PubMed * Google Scholar * Christian Schultheis3, 4 Search for this author in: * NPG journals * PubMed * Google Scholar * Alexander Gottschalk3, 4 Contact Alexander Gottschalk Search for this author in: * NPG journals * PubMed * Google Scholar * Hang Lu1, 2 Contact Hang Lu Search for this author in: * NPG journals * PubMed * Google Scholar * Affiliations * Contributions * Corresponding authorsJournal name:Nature MethodsVolume: 8,Pages:153–158Year published:(2011)DOI:doi:10.1038/nmeth.1555Received13 August 2010Accepted16 December 2010Published online16 January 2011 Abstract * Abstract * Author information * Supplementary information Article tools * Full text * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg The ability to optically excite or silence specific cells using optogenetics has become a powerful tool to interrogate the nervous system. Optogenetic experiments in small organisms have mostly been performed using whole-field illumination and genetic targeting, but these strategies do not always provide adequate cellular specificity. Targeted illumination can be a valuable alternative but it has only been shown in motionless animals without the ability to observe behavior output. We present a real-time, multimodal illumination technology that allows both tracking and recording the behavior of freely moving C. elegans while stimulating specific cells that express channelrhodopsin-2 or MAC. We used this system to optically manipulate nodes in the C. elegans touch circuit and study the roles of sensory and command neurons and the ultimate behavioral output. This technology enhances our ability to control, alter, observe and investigate how neurons, muscles and circuits ultimat! ely produce behavior in animals using optogenetics. View full text Figures at a glance * Figure 1: Illumination system for live animal tracking and optogenetic stimulation and quantification of behavior elicited by targeted illumination. () Optical configuration for using a projector for illumination. The normal epifluorescence optical train is replaced by a projector and a relay lens. Projector image planes are indicated, and a motorized x-y translational stage is used to track animals. () Modification of the three-color LCD projector to further narrow the spectrum is accomplished by the addition of filters into the individual RGB light paths. () Sequential frames from Supplementary Videos 1 and 2 showing qualitative behavioral responses. Top, use of the dorsal coiling effect to cause a worm to crawl in a triangle; bottom, direct muscular control of a paralyzed worm. Images are false-colored to show illumination pattern. () Illustration of the positions of the six sensory neurons, and a frame from Supplementary Video 3 showing the 20-μm bar of blue light, perpendicular to the worm's longitudinal axis, which was scanned at a rate of 12.5% body length per second (~100 μm s−1). () Two scanning schemes alon! g the A-P axis: head to tail and tail to head. () Histograms showing the distributions of positions along the A-P axis where the blue light elicited a reversal response. Shown are the distribution of positions where accelerations elicited by the tail-to-head scan were observed (28 out of 52 worms showed an increase in speed 2 s.d. greater than the average speed before illumination) and the distributions of the anatomical positions of the touch neurons in pmec-4GFP worms. Scale bars, 100 μm. * Figure 2: Optical stimulation of anterior/posterior mechanosensory neurons or forward/backward command interneurons. () Illustration of the positions of neurons expressing ChR2 in pmec-4ChR2 and pglr-1ChR2 transgenic worms. () The touch circuit, showing receptors, command neurons and the resulting behaviors. () Average velocity plots of pmec-4ChR2 worms under illumination conditions (shown as a blue bar above). n = 13 (posterior illumination); n = 15 (anterior illumination). Error bars, s.e.m. () Average velocity plots of pglr-1ChR2 worms under illumination conditions (shown as a blue bar above). n = 24 (posterior illumination); n = 12 (anterior illumination). Error bars. s.e.m. * Figure 3: Quantification of behavioral responses elicited by different anterior illumination intensities. () Patterns used for illumination location and their intensity. () Velocity plots from pooled data from worms receiving different illumination intensities (also see Supplementary Video 5). NR, no response; Sl/P, a slowing or pausing of the worm with no negative velocity; r, a small reversal; R, a large reversal. n = 40 for each of the three illumination levels. The number of worms showing NR, Sl/P, r and R behaviors were 28, 14, 35 and 43 respectively. Error bars, s.e.m. () Distribution of the four responses observed at the three intensity levels. * Figure 4: Illumination patterns used to explore the integration of anterior and posterior signals and behavior generated from the stimulation. () Illumination locations and plot of the temporal variation of the intensity for the two patterns tested. Normalized intensity of 1 corresponds to blue light of intensity 1.17 mW mm−2. () Histogram distributions of intensity at which worms initiated a reversal under two illumination patterns: anterior alone, and anterior and posterior simultaneously (n = 40 for each illumination scheme). () Distributions among the four response states for anterior illumination alone or simultaneous anterior and posterior illumination at the same intensity (1.17mW mm−2) (n = 40 for each). * Figure 5: Simultaneous two-color illumination. () Illustrations of the two illumination schemes. () Velocity plots of pmec-4ChR2 and pglr-1MACmCherry worms subjected to the illumination schemes in . Error bars, s.e.m.; n = 19 for scheme 1, n = 12 for scheme 2. () The neural gentle touch circuit showing the neurons that are either stimulated or silenced and the resulting behaviors at different points in the two sets of experiments. Author information * Abstract * Author information * Supplementary information Affiliations * School of Chemical & Biomolecular Engineering, Georgia Institute of Technology, Atlanta, Georgia, USA. * Jeffrey N Stirman & * Hang Lu * Interdisciplinary Program in Bioengineering, Institute of Biosciences and Bioengineering, Georgia Institute of Technology, Atlanta, Georgia, USA. * Jeffrey N Stirman, * Matthew M Crane & * Hang Lu * Johann Wolfgang Goethe University, Institute of Biochemistry, Biocenter N220, Frankfurt, Germany. * Steven J Husson, * Sebastian Wabnig, * Christian Schultheis & * Alexander Gottschalk * Frankfurt Institute for Molecular Life Sciences, Johann Wolfgang Goethe University, Frankfurt, Germany. * Steven J Husson, * Sebastian Wabnig, * Christian Schultheis & * Alexander Gottschalk Contributions J.N.S., M.M.C., A.G. and H.L. designed the experiments. J.N.S. and M.M.C. wrote the software. J.N.S. constructed the illumination system, performed experiments and analyzed the data. S.J.H., S.W. and C.S. contributed to reagents and provided valuable discussions. J.N.S., M.M.C., S.J.H., A.G. and H.L. prepared the manuscript. Competing financial interests The authors declare no competing financial interests. Corresponding authors Correspondence to: * Alexander Gottschalk or * Hang Lu Supplementary information * Abstract * Author information * Supplementary information Movies * Supplementary Video 1 (176K) Using the dorsal coiling effect and head illumination to dictate the locomotive path of an animal expressing ChR2 in the cholinergic motor neurons. False color recreation was overlaid to show stimulation location and timing. * Supplementary Video 2 (664K) Direct muscular control of a paralyzed worm using light. Worms expressing ChR2 in the muscle cells were paralyzed with an ivermectin solution (0.01 mg ml-1) and were controlled using structured illumination. False color recreation was overlaid to show stimulation location and timing. * Supplementary Video 3 (1M) Illumination line scans performed on freely behaving pmec-4::ChR2 animals eliciting acceleration or reversal behavior depending on the location of illumination. The line scan travels from posterior to anterior and, in separate experiments, anterior to posterior at ~100 μm s-1. Simultaneous blue and red light was used in order to visualize the location of illumination. * Supplementary Video 4 (2M) Using localized light stimulation to excite anterior or posterior gentle touch neurons (in animals carrying pmec-4::ChR2), and anterior or posterior command interneurons (in animals carrying pglr-1::ChR2). False color recreation was overlaid to show stimulation location and timing. * Supplementary Video 5 (2M) Examples of four response states ('NR', 'Sl/P', 'r', 'R') to optical stimulation of the anterior gentle touch neurons (pmec-4::ChR2). False color recreation was overlaid to show stimulation location and timing. * Supplementary Video 6 (1M) Demonstration of complex illumination patterns to investigate sensory integration in pmec-4::ChR2 animals: light pulses of gradually increasing intensity were delivered to the anterior touch neurons, and in a separate experiment the same pulses delivered anteriorly while the posterior touch neurons were continuously illuminated. False color recreation was overlaid to show stimulation location and timing. * Supplementary Video 7 (396K) At certain anterior and posterior illumination intensities the behavior response (forward and reverse locomotion) alternate (in animals carrying pmec-4::ChR2). False color recreation was overlaid to show stimulation location and timing. * Supplementary Video 8 (2M) Using two-color, spatially distinct optical stimuli to rapidly curtail touch avoidance behavior in animals carrying pmec-4::ChR2 and plgr-1::MAC::mCherry. Also shown is the inhibition of a spontaneous reversal, demonstrating that natural, and not merely optogenetically generated reversals, can be inhibited. False color recreation was overlaid to show stimulation location and timing. Zip files * Supplementary Software (3M) Software used for tracking and illumination control. PDF files * Supplementary Text and Figures (780K) Supplementary Figures 1–6 and Supplementary Notes 1–2 Additional data
  • Knocking out multigene redundancies via cycles of sexual assortment and fluorescence selection
    - Nat Meth 8(2):159-164 (2011)
    Nature Methods | Article Knocking out multigene redundancies via cycles of sexual assortment and fluorescence selection * Yo Suzuki1, 11 Contact Yo Suzuki Search for this author in: * NPG journals * PubMed * Google Scholar * Robert P St Onge2 Search for this author in: * NPG journals * PubMed * Google Scholar * Ramamurthy Mani1 Search for this author in: * NPG journals * PubMed * Google Scholar * Oliver D King1, 11 Search for this author in: * NPG journals * PubMed * Google Scholar * Adrian Heilbut3 Search for this author in: * NPG journals * PubMed * Google Scholar * Vyacheslav M Labunskyy4 Search for this author in: * NPG journals * PubMed * Google Scholar * Weidong Chen1 Search for this author in: * NPG journals * PubMed * Google Scholar * Linda Pham1 Search for this author in: * NPG journals * PubMed * Google Scholar * Lan V Zhang1 Search for this author in: * NPG journals * PubMed * Google Scholar * Amy H Y Tong5 Search for this author in: * NPG journals * PubMed * Google Scholar * Corey Nislow6 Search for this author in: * NPG journals * PubMed * Google Scholar * Guri Giaever7 Search for this author in: * NPG journals * PubMed * Google Scholar * Vadim N Gladyshev4 Search for this author in: * NPG journals * PubMed * Google Scholar * Marc Vidal8, 9 Search for this author in: * NPG journals * PubMed * Google Scholar * Peter Schow10 Search for this author in: * NPG journals * PubMed * Google Scholar * Joseph Lehár3 Search for this author in: * NPG journals * PubMed * Google Scholar * Frederick P Roth1, 8, 11 Contact Frederick P Roth Search for this author in: * NPG journals * PubMed * Google Scholar * Affiliations * Contributions * Corresponding authorsJournal name:Nature MethodsVolume: 8,Pages:159–164Year published:(2011)DOI:doi:10.1038/nmeth.1550Received18 October 2010Accepted08 December 2010Published online09 January 2011 Abstract * Abstract * Author information * Supplementary information Article tools * Full text * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg Phenotypes that might otherwise reveal a gene's function can be obscured by genes with overlapping function. This phenomenon is best known within gene families, in which an important shared function may only be revealed by mutating all family members. Here we describe the 'green monster' technology that enables precise deletion of many genes. In this method, a population of deletion strains with each deletion marked by an inducible green fluorescent protein reporter gene, is subjected to repeated rounds of mating, meiosis and flow-cytometric enrichment. This results in the aggregation of multiple deletion loci in single cells. The green monster strategy is potentially applicable to assembling other engineered alterations in any species with sex or alternative means of allelic assortment. To test the technology, we generated a single broadly drug-sensitive strain of Saccharomyces cerevisiae bearing precise deletions of all 16 ATP-binding cassette transporters within clades as! sociated with multidrug resistance. View full text Figures at a glance * Figure 1: Design of the green monster process. () Schematic overview of the process. In yeast, crossing different haploid single mutants generates no-deletion (off-white), one-deletion (light green) and two-deletion (dark green) cells. From this mixture, flow cytometry is used to enrich for two-deletion cells. Higher-order multimutants are assembled via repeated rounds of sexual assortment and enrichment. () In this process a universal GFP deletion cassette replaces KanMX4 in a target gene (yfg) via recombination within Kan subsequences internal to the flanking barcodes. The inducible tetO2 promoter allows titration of GFP expression. Transcriptional terminators (brown) and the Kan promoter (light blue) and terminator (dark blue), each derived from the Ashbya gossypii TEF gene, are shown. The transformation marker is URA3. () GMToolkits, inserted at the CAN1 locus, contain rtTA21 and either KanMX4 and STE2pr-Sp-his5 (GMToolkit-) or NatMX420 and STE3pr-LEU2 (ref. 19) (GMToolkit-α). * Figure 2: Demonstration of the green monster process. () Simulations showing that >99% of a cell population accumulate all 24 deletions in eight (top), 12 (middle) or 19 rounds (bottom), with greater efficiency for lower coefficient of variation (CV) of GFP signal intensity (achievable using internal standard to control for noise). () Simulation showing that 24 linked deletions with the meiotic cross-over probability between adjacent loci of 5% can be assembled in 16 rounds when the GFP signal intensity CV is 50%. () Histograms illustrating the results of cell sorting for no-GFP cells (0Δ), single-GFP cells (1Δ) and a haploid 'meiotic mix' resulting from a cross of two single-GFP strains, with an expected 1:2:1 ratio of no-GFP, one-GFP and two-GFP (2Δ) cells. The brightest 1% of the cells in the meiotic mix were collected (red filled area). () GFP fluorescence intensity (arbitrary units) of multimutants. Histograms are shown for no-GFP, 1-GFP, 2-GFP, 4-GFP, 8-GFP and 16-GFP 'ABC16-monster' cells (isogenic populations). () Fl! uorescence micrographs showing nonmutant cells, double-mutant cells, ABC16-monster cells, and a mixture of double-mutant and ABC16-monster cells. Identical exposure, brightness, and contrast settings were used for images. Scale bar, 10 μm. (). Average deletion numbers for the en masse green monster process from three independent processes are plotted. Error bars, s.d. From Round 1 to Round 5, n = 21, 23, 24, 24, 24 (red); n = 23, 24, 24, 24, 23 (blue); n = 24, 24, 23, 24, 34 (brown). * Figure 3: Hypersensitivity of the ABC16 monster to drugs. () Number of drugs to which the ABC16 monster or the previously described drug-hypersensitive AD strain is sensitive compared to wild type. () IC50 values for single-mutant drug sensitivity and for ABC16-monster drug sensitivity relative to that of the corresponding nonmutant-drug combination as indicated in the legend (top). The minimum value among the relative IC50 values for single mutants is indicated for comparison with the relative IC50 of the ABC16 monster. () Exponential growth rates of the ABC16-monster (green), nonmutant (blue) and single-deletion strains (gray) as a function of tamoxifen, fluconazole and valinomycin concentration. Author information * Abstract * Author information * Supplementary information Affiliations * Department of Biological Chemistry and Molecular Pharmacology, Harvard Medical School, Boston, Massachusetts, USA. * Yo Suzuki, * Ramamurthy Mani, * Oliver D King, * Weidong Chen, * Linda Pham, * Lan V Zhang & * Frederick P Roth * Stanford Genome Technology Center, Palo Alto, California, USA. * Robert P St Onge * Bioinformatics Program, Boston University, Boston, Massachusetts, USA. * Adrian Heilbut & * Joseph Lehár * Division of Genetics, Brigham and Women's Hospital, Harvard Medical School, Boston, Massachusetts, USA. * Vyacheslav M Labunskyy & * Vadim N Gladyshev * Genome Research Centre, The University of Hong Kong, Pokfulam, Hong Kong, China. * Amy H Y Tong * Department of Molecular Genetics, Donnelly Centre for Cellular and Biomolecular Research, University of Toronto, Toronto, Ontario, Canada. * Corey Nislow * Department of Pharmaceutical Sciences, Department of Molecular Genetics, Donnelly Centre for Cellular and Biomolecular Research, University of Toronto, Toronto, Ontario, Canada. * Guri Giaever * Center for Cancer Systems Biology, Dana-Farber Cancer Institute, Boston, Massachusetts, USA. * Marc Vidal & * Frederick P Roth * Department of Genetics, Harvard Medical School, Boston, Massachusetts, USA. * Marc Vidal * Flow Cytometry Core Facility, Dana-Farber Cancer Institute, Boston, Massachusetts, USA. * Peter Schow * Present addresses: Department of Synthetic Biology and Bioenergy, J. Craig Venter Institute, San Diego, California, USA (Y.S.), Boston Biomedical Research Institute, Watertown, Massachusetts, USA (O.D.K.) and Donnelly Centre for Cellular and Biomolecular Research, University of Toronto and Samuel Lunenfeld Research Institute, Mt. Sinai Hospital, Toronto, Ontario, Canada (F.P.R.). * Yo Suzuki, * Oliver D King & * Frederick P Roth Contributions Y.S. and F.P.R. developed the green monster method and prepared the manuscript; R.P.S.O., A.H., J.L. and Y.S. measured drug sensitivity; R.M. analyzed growth curves; O.D.K. simulated the process; L.V.Z., C.N. and G.G. advised on method design; A.H.Y.T., V.M.L., V.N.G. and M.V. provided reagents and advice; W.C. and L.P. provided technical support; P.S. and Y.S. performed flow cytometry. Competing financial interests The authors declare no competing financial interests. Corresponding authors Correspondence to: * Yo Suzuki or * Frederick P Roth Supplementary information * Abstract * Author information * Supplementary information PDF files * Supplementary Text and Figures (4M) Supplementary Figures 1–8 and Supplementary Tables 1–13 Additional data
  • A transgenic mouse for in vivo detection of endogenous labeled mRNA
    - Nat Meth 8(2):165-170 (2011)
    Nature Methods | Article A transgenic mouse for in vivo detection of endogenous labeled mRNA * Timothée Lionnet1, 2 Search for this author in: * NPG journals * PubMed * Google Scholar * Kevin Czaplinski1, 5 Search for this author in: * NPG journals * PubMed * Google Scholar * Xavier Darzacq3 Search for this author in: * NPG journals * PubMed * Google Scholar * Yaron Shav-Tal4 Search for this author in: * NPG journals * PubMed * Google Scholar * Amber L Wells1, 5 Search for this author in: * NPG journals * PubMed * Google Scholar * Jeffrey A Chao1 Search for this author in: * NPG journals * PubMed * Google Scholar * Hye Yoon Park1, 2 Search for this author in: * NPG journals * PubMed * Google Scholar * Valeria de Turris1 Search for this author in: * NPG journals * PubMed * Google Scholar * Melissa Lopez-Jones1 Search for this author in: * NPG journals * PubMed * Google Scholar * Robert H Singer1, 2 Contact Robert H Singer Search for this author in: * NPG journals * PubMed * Google Scholar * Affiliations * Contributions * Corresponding authorJournal name:Nature MethodsVolume: 8,Pages:165–170Year published:(2011)DOI:doi:10.1038/nmeth.1551Received23 September 2010Accepted10 December 2010Published online16 January 2011 Abstract * Abstract * Author information * Supplementary information Article tools * Full text * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg Live-cell single mRNA imaging is a powerful tool but has been restricted in higher eukaryotes to artificial cell lines and reporter genes. We describe an approach that enables live-cell imaging of single endogenous labeled mRNA molecules transcribed in primary mammalian cells and tissue. We generated a knock-in mouse line with an MS2 binding site (MBS) cassette targeted to the 3′ untranslated region of the essential ββ-actin gene. As β-actin–MBS was ubiquitously expressed, we could uniquely address endogenous mRNA regulation in any tissue or cell type. We simultaneously followed transcription from the β-actin alleles in real time and observed transcriptional bursting in response to serum stimulation with precise temporal resolution. We tracked single endogenous labeled mRNA particles being transported in primary hippocampal neurons. The MBS cassette also enabled high-sensitivity fluorescence in situ hybridization (FISH), allowing detection and localization of single ! β-actin mRNA molecules in various mouse tissues. View full text Figures at a glance * Figure 1: Schematic of the Actb-MS2 system for live-cell imaging. () As the gene is transcribed by the RNA polymerase (RNAP), the RNA hairpins form and get bound by the coexpressed MCP-YFP. () In the MBS cassette, a unit containing two MBS sequences and the intervening linkers is repeated 12 times, resulting in 24 MBSs. We designed three FISH probes (named Lk51-1, Lk20 and Lk51-2) that bind each unit at the indicated positions. The MBS array is inserted downstream of the zip code regulatory region (green). () In the construct (top), the long homology arm (LA) encompasses the full Actb gene, including a region 4 kbp upstream of the transcription start site (TSS); the positions of the exons (blue), introns (gray), start and stop codon, and polyadenylation site (poly(A)) are indicated. The short homology arm (SA) extends 1.3 kbp downstream of the Neo cassette (yellow) flanked by the two lox sites (purple triangles). The 24× MBS cassette (red) is inserted in the 3′ UTR in the sixth exon. The resulting genomic locus in the Actb–MBS mouse i! s shown on the bottom. * Figure 2: RNA FISH in sections from various tissues. (–) Merge of DAPI signal (blue) and Cy5 fluorescence from three FISH probes targeting the MBS cassette (red; bandpass data) in the indicated tissues from the indicated strains. Scale bars, 10 μm (–), 5 μm (–; magnification of boxed areas in –). () Quantification of the Actb-MBS allele expression (number of spots counted) in the cerebellum after thresholding the FISH signal. () Average mRNA concentration inside the nucleus (left) and outside the nucleus, displayed as a function of the distance from the nuclear boundary (right). Both concentrations were normalized to their value at the nucleus boundary. AU, arbitrary units. * Figure 3: Actb mRNA localizes to the leading edge of primary fibroblasts isolated from MBS mice. (–) Differential interference contrast image (), DAPI-stained image (), FISH with Cy3-labeled probes to the Actb coding region () and FISH with Cy5-labeled probes to the MBS cassette. () Scale bar, 10 μm. () Time-lapse images of a primary fibroblast migrating on a fibronectin substrate. Cells were infected with lentivirus that expresses NLS-MCP-GFP, and stained with membrane-permeant red cytoplasmic dye. Color bar, NLS-MCP-GFP fluorescence normalized by the red cytoplasmic dye intensity to account for the cell volume. AU, arbitrary units. Scale bar, 20 μm. * Figure 4: Live-cell imaging of serum response in MBS immortalized MEFs. () Images of immortalized MEFs (tetraploids) during serum response taken at indicated times after serum addition (maximum intensity projections of z-dimension stacks). At 0 min, no transcriptional activity was detected, and at subsequent time points all four transcription sites appeared as bright nuclear spots (arrows). Scale bar, 5 μm. () Quantification of the fluorescence intensity at the transcription sites marked in . Black, average response of the four alleles in . Gray, average response over 11 cells. (–) Data from shown separately for each allele. AU, arbitrary units. * Figure 5: Live-cell imaging of mRNP transport in primary hippocampal neurons. (–) Images of neurons transfected with a plasmid encoding MCP-YFP (imaged at 20 frames s−1; shown images are 1 s apart) showing an mRNP moving unidirectionally along a neuronal process. Scale bar, 10 μm. () Trajectories of two particles (circles and squares) observed successively along the process shown in –. () Instantaneous rates for both mRNPs (averages ± s.e.m., 2.95 ± 0.14 μm s−1 (circles) and 2.90 ± 0.13 μm s−1 (squares)). Author information * Abstract * Author information * Supplementary information Affiliations * Department of Anatomy and Structural Biology, Albert Einstein College of Medicine, Bronx, New York, USA. * Timothée Lionnet, * Kevin Czaplinski, * Amber L Wells, * Jeffrey A Chao, * Hye Yoon Park, * Valeria de Turris, * Melissa Lopez-Jones & * Robert H Singer * Gruss Lipper Biophotonics Center, Albert Einstein College of Medicine, Bronx, New York, USA. * Timothée Lionnet, * Hye Yoon Park & * Robert H Singer * Institut de Biologie de l'Ecole Normale Supérieure, Centre National de la Recherche Scientifique Unité Mixte de Recherche 8197, Paris, France. * Xavier Darzacq * The Mina and Everard Goodman Faculty of Life Sciences & Institute of Nanotechnology and Advanced Materials, Bar-Ilan University, Ramat Gan, Israel. * Yaron Shav-Tal * Present addresses: Department of Biochemistry and Cell Biology, Center for Nervous Systems Disorders, Stony Brook University Stony Brook, New York, USA (K.C.) and Department of Medicine, Albert Einstein College of Medicine, Bronx, New York, USA (A.L.W.). * Kevin Czaplinski & * Amber L Wells Contributions T.L. performed the biochemistry experiments, the tissue FISH imaging, serum response live-cell imaging, and quantitative mRNA FISH, analyzed the data and wrote the paper. K.C. generated cell lines and performed the neuron live-cell imaging. X.D. and Y.S.-T. generated the mouse line. A.L.W. performed FISH mRNA localization experiments. J.A.C. performed the serum response live-cell imaging. H.Y.P. performed the live-cell localization experiments. V.d.T. generated cell lines. M.L.-J. performed the biochemistry experiments. R.H.S. consulted on the research and helped write the paper. Competing financial interests The authors declare no competing financial interests. Corresponding author Correspondence to: * Robert H Singer Supplementary information * Abstract * Author information * Supplementary information Movies * Supplementary Video 1 (1M) Live-cell imaging of a serum-induced primary fibroblast. MCP-GFP-labeled mRNA particles can be detected moving around the cell; the two transcription sites of the primary cell appear as two bright spots in the nucleus. Note that the transcription sites intensity is intentionally saturated to allow visualizing the dimmer single particles. * Supplementary Video 2 (2M) Individual mRNP moving along a neuronal process. * Supplementary Video 3 (2M) Individual mRNP moving along a neuronal process. The process is the same as the one imaged in Supplementary Video 2. * Supplementary Video 4 (236K) Anterograde mRNP motion along a neuronal process. * Supplementary Video 5 (212K) Retrograde mRNP motion along a neuronal process. * Supplementary Video 6 (2M) Bidirectional mRNP motion along a neuronal process. * Supplementary Video 7 (2M) Branching mRNP motion along a neuronal process. * Supplementary Video 8 (928K) Immobile mRNP in a neuronal process. PDF files * Supplementary Text and Figures (1M) Supplementary Figures 1–8, Supplementary Note 1 Additional data
  • A microfluidic array for large-scale ordering and orientation of embryos
    - Nat Meth 8(2):171-176 (2011)
    Nature Methods | Article A microfluidic array for large-scale ordering and orientation of embryos * Kwanghun Chung1, 3 Search for this author in: * NPG journals * PubMed * Google Scholar * Yoosik Kim2, 3 Search for this author in: * NPG journals * PubMed * Google Scholar * Jitendra S Kanodia2 Search for this author in: * NPG journals * PubMed * Google Scholar * Emily Gong1 Search for this author in: * NPG journals * PubMed * Google Scholar * Stanislav Y Shvartsman2 Search for this author in: * NPG journals * PubMed * Google Scholar * Hang Lu1 Contact Hang Lu Search for this author in: * NPG journals * PubMed * Google Scholar * Affiliations * Contributions * Corresponding authorJournal name:Nature MethodsVolume: 8,Pages:171–176Year published:(2011)DOI:doi:10.1038/nmeth.1548Received04 October 2010Accepted29 November 2010Published online26 December 2010 Abstract * Abstract * Author information * Supplementary information Article tools * Full text * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg Quantitative studies of embryogenesis require the ability to monitor pattern formation and morphogenesis in large numbers of embryos, at multiple time points and in diverse genetic backgrounds. We describe a simple approach that greatly facilitates these tasks for Drosophila melanogaster embryos, one of the most advanced models of developmental genetics. Based on passive hydrodynamics, we developed a microfluidic embryo-trap array that can be used to rapidly order and vertically orient hundreds of embryos. We describe the physical principles of the design and used this platform to quantitatively analyze multiple morphogen gradients in the dorsoventral patterning system. Our approach can also be used for live imaging and, with slight modifications, could be adapted for studies of pattern formation and morphogenesis in other model organisms. View full text Figures at a glance * Figure 1: Microfluidic embryo-trap array for high-throughput arraying of vertically oriented Drosophila embryos. () Image of an adult Drosophila (left) with dorsal, posterior, ventral and anterior directions indicated. Scale bar, 1 mm. () Micrograph of early embryo stained using antibody to Dl. (Anterior is to the left, and dorsal is at the top.) Scale bar, 100 μm. () Photograph of the device (left) and a micrograph of the boxed region (right). Scale bar, 1 cm (left) and 500 μm (right). () Detail of the embryo-trap array design (top view). () Scanning electron micrograph of the trap structure. Scale bar, 100 μm. () Schematic showing the embryo trapping process: an embryo is guided into the trap (top); the flow around the embryo orients it vertically (middle); the trap contracts and secures the embryo (bottom). The yellow plane represents imaging focal plane. Blue arrows show the direction of bulk flow in the serpentine channel. () Schematic of the imaging setup. Inset, representative confocal image of an embryo stained with antibodies to Dl, Twist and dpERK. () A section of the arra! y with trapped embryos (dark circular object in each trap). Scale bar, 500 μm. * Figure 2: Operating principles of the embryo-trap array. (,) Volumetric flow rate in the serpentine main channel () and through the cross-flow channels () at each trap. Widths of the resistance channels in the optimal design (Fig. 1d), low-resistance design and high resistance design were 40 μm, 80 μm and 20 μm, respectively. Dummy columns are the first and last columns of the device. () Schematic of streamlines plotted from the numerical computational fluid dynamic model as the fluid turns the corner in the main channel. () Optical images at the indicated time points show an embryo (circled) migrating along the wall of the serpentine channel. Scale bar, 800 μm. (–) Three-dimensional characterization of the trap by confocal microscopy at 0 psi (–) and 6 psi (–). Single-frame top view from the middle of the device (,; dotted red circle represents dorsoventral plane of an embryo). Single frame cross-sectional view of the trap opening (,; dotted red ellipse represents vertically oriented embryo). Dotted white lines, locatio! ns where cross-sections of the trap opening (,) were acquired. Scale bars, 100 μm. * Figure 3: Spatial extent of the Dl gradient. () Confocal images of vertically oriented embryos stained for Dl and stained with DAPI. A merge is also shown. (–) Average gradients of nuclear Dl from four representative experiments. Error bars are s.e.m. (number of gradients used is indicated in each plot). The arrow denotes the dorsoventral (DV) position beyond which the nuclear Dl gradient can be considered 'flat'. DV distances are normalized: x = 0 for ventral and x = 1 for dorsal. (,) Early () and late () expression patterns of Dl and zen. () Schematic of regulatory models that can be used to account for the two phases of zen expression (top schematic depicts early expression). U is a uniform activator and pMAD is phosphorylated MAD. (–) Pairwise comparison of Dl gradients in wild-type and mutant backgrounds. Nuclear Dl gradients from the wild-type embryos (), embryos from dl−/+ females (), and average gradients for both genetic backgrounds (). Error bars, s.e.m. (n = 70 for wild type and n = 82 for mutant). * Figure 4: Quantitative characterization of signal transduction and morphogen gradients in dorsoventral patterning. () Schematic of the dorsoventral patterning network, showing the feedforward loops activated by Dl. (–) Confocal images of embryos immunostained for Dl and Twist (Twi) (), Dl and phospho-MAPK (dpERK) (), and Dl and phospho-MAD (pMAD) (). Scale bar, 25 μm. (–) Averaged gradients of pMAD (), Twi () and dpERK (). Error bars, s.e.m. (n = 64 gradients (), 40 gradients () and 38 gradients (), respectively). * Figure 5: Live imaging of embryos using the embryo array. (,) Frames from videos of embryos expressing nuclear histone– GFP undergoing nuclear divisions () or ventral invagination (). For both videos, images were taken 70 μm from the anterior pole. Scale bars, 25 μm. Author information * Abstract * Author information * Supplementary information Primary authors * These authors contributed equally to this work. * Kwanghun Chung & * Yoosik Kim Affiliations * School of Chemical and Biomolecular Engineering, and Parker H. Petit Institute for Bioengineering and Bioscience, Georgia Institute of Technology, Atlanta, Georgia, USA. * Kwanghun Chung, * Emily Gong & * Hang Lu * Department of Chemical and Biological Engineering and Lewis-Sigler Institute for Integrative Genomics, Princeton University, Princeton, New Jersey, USA. * Yoosik Kim, * Jitendra S Kanodia & * Stanislav Y Shvartsman Contributions K.C., E.G. and H.L. designed, fabricated and tested the device. Y.K. tested the device and performed imaging. J.S.K. wrote the image processing and statistical analysis programs for gradient quantification. K.C., Y.K., S.Y.S. and H.L. designed the experiments and wrote the paper. Competing financial interests The authors declare no competing financial interests. Corresponding author Correspondence to: * Hang Lu Supplementary information * Abstract * Author information * Supplementary information Movies * Supplementary Video 1 (3M) Drosophila embryo trapping. This movie shows trapping of the embryos from an embryo suspension. * Supplementary Video 2 (340K) Contraction of the traps. This movie shows automatic contraction of the traps resulting from the loading pressure being decreased from 6 psi to 0 psi. Notice that embryos in the traps are not secured. * Supplementary Video 3 (3M) Live imaging: early embryo. This movie shows consecutive nuclear divisions in the early embryo. * Supplementary Video 4 (996K) Live imaging: ventral invagination. This movie shows consecutive nuclear divisions in an embryo undergoing ventral invagination. PDF files * Supplementary Text and Figures (508K) Supplementary Figures 1– 4 Additional data
  • Efficient modeling, simulation and coarse-graining of biological complexity with NFsim
    - Nat Meth 8(2):177-183 (2011)
    Nature Methods | Article Efficient modeling, simulation and coarse-graining of biological complexity with NFsim * Michael W Sneddon1, 2 Search for this author in: * NPG journals * PubMed * Google Scholar * James R Faeder3 Search for this author in: * NPG journals * PubMed * Google Scholar * Thierry Emonet1, 2, 4 Contact Thierry Emonet Search for this author in: * NPG journals * PubMed * Google Scholar * Affiliations * Contributions * Corresponding authorJournal name:Nature MethodsVolume: 8,Pages:177–183Year published:(2011)DOI:doi:10.1038/nmeth.1546Received08 September 2010Accepted03 December 2010Published online26 December 2010 Abstract * Abstract * Author information * Supplementary information Article tools * Full text * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg Managing the overwhelming numbers of molecular states and interactions is a fundamental obstacle to building predictive models of biological systems. Here we introduce the Network-Free Stochastic Simulator (NFsim), a general-purpose modeling platform that overcomes the combinatorial nature of molecular interactions. Unlike standard simulators that represent molecular species as variables in equations, NFsim uses a biologically intuitive representation: objects with binding and modification sites acted on by reaction rules. During simulations, rules operate directly on molecular objects to produce exact stochastic results with performance that scales independently of the reaction network size. Reaction rates can be defined as arbitrary functions of molecular states to provide powerful coarse-graining capabilities, for example to merge Boolean and kinetic representations of biological networks. NFsim enables researchers to simulate many biological systems that were previously ! inaccessible to general-purpose software, as we illustrate with models of immune system signaling, microbial signaling, cytoskeletal assembly and oscillating gene expression. View full text Figures at a glance * Figure 1: Combinatorial complexity in multisite phosphorylation and NFsim performance scaling. () A substrate protein (S, blue) can be phosphorylated (P, red) at multiple independent sites by a kinase (K, yellow). A single rule, indicating that a site named 'p' on 'S' must be in the unphosphorylated state 'U' for the event to occur, can represent 4n–1 different reactions, where n is the number of phosphorylation sites on the substrate protein. () The number of reactions and chemical species that need to be accounted for grows exponentially with n. Rules and parameters grow only linearly with n. () The runtime performance of NFsim (blue filled circles) for this model is compared to the runtime of optimized ODE (triangles) and SSA (open circles) simulators9, 10. Network generation (squares) depicts the computational cost of transforming a rule-based model into a set of reactions that can be simulated by ODE or SSA simulators. * Figure 2: Schematic overview of NFsim. () Rules keep track of the molecular agents that can participate in a reaction (dashed lines) by matching possible reactants to user-defined reactant patterns. At each simulation step, a rule event is generated, reactant molecules are selected and transformed, and the set of possible reactants for each rule is updated (see Online Methods). In addition to the binding and unbinding events, rules can also specify reversible reactions, domain state changes, molecular synthesis and molecular degradation. () Example BNGL file specifying the model depicted in . Lines that begin with # are user comments ignored by NFsim. Parameters and rate constants are defined in the parameters block. Molecule types 'A', 'B' and 'C' are defined with a set of labeled domains 'a', 'b' and 'c'. Observables specify molecular patterns that provide simulation output, such as the pattern 'AB_complex'. Molecular domains are referenced in rules to define how molecules interact. 'A(b!1).B(a!1)' denotes that! a bond connects domain 'b' of molecule 'A' to domain 'a' of molecule 'B'. Here binding of 'A' to 'B' is declared to be independent of the binding of 'A' to 'C', because in the reactant pattern of the rule, the site named 'c' of molecule 'A' is omitted. Reaction rates are given as parameters 'k1', 'k2' and 'k3'. * Figure 3: Simulation performance and parameter estimation for receptor aggregation models. () Schematic of the early events of Fcε receptor (FcεRI) signaling. () The runtime performance of NFsim (filled circles) for a compendium of eight FcεRI signaling models of increasing reaction network size27 as compared to ODE simulation (triangles), SSA simulation (open circles) and reaction network generation (squares). We used an optimized ODE solver10 that can activate sparse-matrix representations and adaptive time-steps, leading to the apparent plateau in ODE performance. The largest model could not be simulated with the SSA because total computer memory (4 GB) was exhausted. () The trivalent-ligand, bivalent-receptor (TLBR) model serves as a simplified representation of FcεRI aggregation and is readily encoded in three BNGL rules, where the syntax 'r!+' indicates that the molecular domain named 'r' must be bound. () We used the NFsim suite of Matlab-based utilities to fit the TLBR model parameters to published flow cytometry data30 that measured steady-state recep! tor-ligand binding. * Figure 4: Tracking molecular connectivity during simulation of cytoskeletal actin polymerization. () Simplified versions of the rules that model actin polymerization, branching and severing reactions. (,) Comparison of simulations with TIRF microscopy experiments that monitored filament branching in flow cells32. () Distributions of the positions of branching events taking place on preexisting mother filaments. Distances are measured relative to the position of the barbed end of the mother filament at the time of Arp2/3 addition. () Distributions of the positions of branching events taking place on portions of mother filaments that elongated after addition of Arp2/3. Distances are measured from the branching point to the position of the growing barbed end of the mother filament at the time of branching. Error bars denote s.e.m. (n = 146 for ; n = 154 for ). () Three-dimensional visualizations of the molecular connectivity generated using NFsim's output options depicting ATP-actin subunits (blue), ADP-Pi actin subunits (cyan), ADP actin subunits (red) and filament ends th! at are capped by capping protein (yellow). Inset shows a close-up of the visualization. (,) Simulated trajectory of the mean filament length of a connected actin structure () and corresponding steady-state distribution (). (,) Simulated trajectory of the mean number of branches in a connected actin structure () and corresponding steady-state distribution (). * Figure 5: Coarse-graining with local and global functions. () Active (on) and inactive (off) conformations of signaling teams of chemoreceptor dimers in the bacterial chemotaxis system. The probability of a signaling team being in the active conformation depends on the methylation level m of each receptor in the complex and the concentration of external ligand l (ref. 12). () Local functions use observable patterns to track the methylation state of individual dimers and calculate the probability of each signaling team (x) being active. () The chemotaxis signaling model captures the observed response of the system to increasing doses (arrows) of the chemoattractant methyl-aspartate. () The flagellar motor is modeled as a two-state system in which states correspond to clockwise (CW) or counter-clockwise (CCW) rotation34. The rate of transitions between states depends on the height of the free energy barrier, which varies in time with the concentration of phosphorylated CheY ([CheY-P]). This model is specified with an observable patter! n that tracks CheY-P numbers and global functions that define the rate at which the motor switches states. () The model simulated with NFsim (line) captures the probability of being in the CW rotational state (CW bias) as a function of [CheY-P] as measured in single cell experiments35 (circles); inset shows the free energy diagram governing the transitions between CW and CCW rotations. * Figure 6: Achieving multiple levels of resolution with conditional and functional rate-law expressions. () Schematic diagram of a biochemical system that can oscillate owing to negative feedback with a time delay that arises from nuclear shuttling and protein synthesis. For the system to oscillate, the negative feedback on the promoter activity must show some nonlinearity. () Nonlinearity represented by a simplified Boolean ON-OFF switch, a piecewise linear response or a Hill function. () Functions written in NFsim describing each of these coarse-grained representations. Conditional expressions, which can be arbitrarily nested as shown in the definition of the linear approximation, are interpreted as "if [Condition], then use [RateExpression1], else [RateExpression2]". () Time courses for mRNA (black solid line) and protein (gray dashed line) levels for the different coarse-grained representations. Author information * Abstract * Author information * Supplementary information Affiliations * Department of Molecular, Cellular and Developmental Biology, Yale University, New Haven, Connecticut, USA. * Michael W Sneddon & * Thierry Emonet * Interdepartmental Program in Computational Biology and Bioinformatics, Yale University, New Haven, Connecticut, USA. * Michael W Sneddon & * Thierry Emonet * Department of Computational and Systems Biology, University of Pittsburgh School of Medicine, Pittsburgh, Pennsylvania, USA. * James R Faeder * Department of Physics, Yale University, New Haven, Connecticut, USA. * Thierry Emonet Contributions M.W.S. wrote the software and performed all simulations. M.W.S., J.R.F. and T.E. designed the algorithms and research and wrote the manuscript. Competing financial interests The authors declare no competing financial interests. Corresponding author Correspondence to: * Thierry Emonet Supplementary information * Abstract * Author information * Supplementary information Movies * Supplementary Video 1 (3M) Unconstrained actin growth simulated with NFsim. Visualizations depict ATP-actin subunits (blue), ADP-Pi actin subunits (cyan), ADP actin subunits (red) and filament ends that are capped by capping protein (yellow). In this simulation, the concentration of the ADF/cofilin severing complex is set to zero, which allows the structure to continue rapid growth throughout the simulation. * Supplementary Video 2 (2M) Actin growth in the presence of ADF/cofilin. Visualizations depict ATP-actin subunits (blue), ADP-Pi actin subunits (cyan), ADP actin subunits (red) and filament ends that are capped by capping protein (yellow). In this simulation, a steady-state regime is achieved where branching and polymerization reactions are compensated by the severing of filaments. Severed ends of the filament are discarded from the simulation so that only a single connected structure is followed over time. Notice that actin structures are typically small and consist of only a few filaments that are capped. Occasional stochastic events, however, allow periods of rapid growth and the transient formation of much larger structures. PDF files * Supplementary Text and Figures (1M) Supplementary Figures 1–7, Supplementary Tables 1–7 and Supplementary Notes 1–12 Additional data
  • Addendum: Mechanical regulation of cell function with geometrically modulated elastomeric substrates
    - Nat Meth 8(2):184 (2011)
    Nature Methods | Addendum Addendum: Mechanical regulation of cell function with geometrically modulated elastomeric substrates * Jianping Fu Search for this author in: * NPG journals * PubMed * Google Scholar * Yang-Kao Wang Search for this author in: * NPG journals * PubMed * Google Scholar * Michael T Yang Search for this author in: * NPG journals * PubMed * Google Scholar * Ravi A Desai Search for this author in: * NPG journals * PubMed * Google Scholar * Xiang Yu Search for this author in: * NPG journals * PubMed * Google Scholar * Zhijun Liu Search for this author in: * NPG journals * PubMed * Google Scholar * Christopher S Chen Search for this author in: * NPG journals * PubMed * Google ScholarJournal name:Nature MethodsVolume: 8,Page:184Year published:(2011)DOI:doi:10.1038/nmeth0211-184aPublished online28 January 2011 Article tools * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg Nat. Methods7, 733–736 (2010); published online 1 August 2010; addendum published after print 28 January 2011. In the version of this article initially published, the implication that it was the first work to decouple substrate rigidity from surface properties was incorrect, as we and others had previously reported the approach. Additional reference to previous work on micropost arrays also should have been included1. Our fabrication process, in which micropost arrays are doubly replica molded from microfabricated silicon masters, scales up production of these substrates and allows replication and distribution of disposable molds to potential users. References * Saez, A., Buguin, A., Silberzan, P. & Ladoux, B.Biophys. J.89, L52–L54 (2005). * ChemPort * ISI * PubMed * Article Download references Additional data
  • Corrigendum: Two-photon calcium imaging from head-fixed Drosophila during optomotor walking behavior
    - Nat Meth 8(2):184 (2011)
    Nature Methods | Corrigendum Corrigendum: Two-photon calcium imaging from head-fixed Drosophila during optomotor walking behavior * Johannes D Seelig Search for this author in: * NPG journals * PubMed * Google Scholar * M Eugenia Chiappe Search for this author in: * NPG journals * PubMed * Google Scholar * Gus K Lott Search for this author in: * NPG journals * PubMed * Google Scholar * Anirban Dutta Search for this author in: * NPG journals * PubMed * Google Scholar * Jason E Osborne Search for this author in: * NPG journals * PubMed * Google Scholar * Michael B Reiser Search for this author in: * NPG journals * PubMed * Google Scholar * Vivek Jayaraman Search for this author in: * NPG journals * PubMed * Google ScholarJournal name:Nature MethodsVolume: 8,Page:184Year published:(2011)DOI:doi:10.1038/nmeth0211-184bPublished online28 January 2011 Article tools * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg Nat. Methods7, 535–540 (2010); published online 6 June 2010; corrected after print 10 January 2011. In the version of this article initially published, the units for angular position (degrees) in Figure 3a,b are incorrect. The correct unit should be mm. The error has been corrected in the HTML and PDF versions of the article. Additional data
  • Erratum: Salience
    - Nat Meth 8(2):184 (2011)
    Nature Methods | Erratum Erratum: Salience * Bang Wong Search for this author in: * NPG journals * PubMed * Google ScholarJournal name:Nature MethodsVolume: 8,Page:184Year published:(2011)DOI:doi:10.1038/nmeth0211-184cPublished online28 January 2011 Article tools * Print * Email * Download PDF * Download citation * Order reprints * Rights and permissions * Share/bookmark * Connotea * CiteULike * Facebook * Twitter * Delicious * Digg Nat. Methods7, 773 (2010); published online 29 September 2010; corrected after print 15 December 2010. In the version of this article initially published, a portion of Figure 1 was missing. The error has been corrected in the HTML and PDF versions of the article. Additional data