DOCSLIB.ORG

Fluorescent Probes for RESOLFT-Type Microscopy at Low Light Intensities

Total Page：16

File Type：pdf, Size：1020Kb

Download full-text PDF Read full-text
Fluorescent Probes for RESOLFT-Type Microscopy at Low Light Intensities Generation of Novel Photochromic GFPs: Fluorescent Probes for RESOLFT-type Microscopy at Low Light Intensities Dissertation for the award of the degree “Doctor rerum naturalium” Division of Mathematics and Natural Sciences of the Georg-August-Universität Göttingen submitted by Tim Grotjohann from Hannover Göttingen, 2012 Thesis committee members: - Prof. Dr. Stefan Jakobs (1st Referee) Max Planck Institute for Biophysical Chemistry, Göttingen Department of NanoBiophotonics Mitochondrial Structure and Dynamics Group - Prof. Dr. Kai Tittmann (2nd Referee) Georg August University Göttingen Albrecht von Haller Institute Department of Bioanalytics - Dr. Dieter Klopfenstein Georg August University Göttingen Third Institute of Physics Department of Biophysics Date of oral examination: 18th April, 2012 Affidavit I hereby ensure that the presented thesis “Generation of novel photochromic GFPs: fluorescent probes for live cell RESOLFT-type microscopy at low light intensities” has been written independently and with no other sources and aids than quoted. ___________________________________ (Tim Grotjohann) 10th February 2012, Göttingen Table of Contents I. Summary ............................................................................ 4 II. Introduction ........................................................................ 5 1. Fluorescence Microscopy ................................................................................................ 6 a. Fluorescence ............................................................................................................... 6 b. Fluorescence Microscopy Techniques ........................................................................ 9 c. The Diffraction Barrier and Super-Resolution Microscopy ........................................ 11 2. Fluorescent Proteins ...................................................................................................... 15 a. The Overall Structure of Fluorescent Proteins .......................................................... 16 b. The Chromophore and Its Environment - Maturation, Conformation, Protonation ... 17 c. Tuning the Spectral Properties of Fluorescence Proteins ......................................... 22 d. Optimizing Fluorescent Protein Characteristics for Specific Needs .......................... 25 e. Photoactivatable and Photoconvertable Fluorescent Proteins ................................. 26 f. Reversibly Switchable Fluorescent Proteins ............................................................. 29 III. Aims .................................................................................. 34 IV. Results .............................................................................. 35 1. Generation and Establishment of a Screening System to Study RSFP Characteristics ................................................................................................................ 35 2. Characterization and Comparison of commonly used RSFPs .................................. 38 3. Reversibly Switchable Enhanced Green Fluorescent Protein (rsEGFP) .................. 40 a. Generation of rsEGFP ............................................................................................... 40 b. Determination of rsEGFP Characteristics ................................................................. 41 c. Using rsEGFP as a Rewritable Data Storage Medium ............................................. 47 d. Establishing a RESOLFT-type Microscopy Approach Using rsEGFP ...................... 49 e. Establishing a Diffraction-Unlimited all Optical Data Storage Approach ................... 53 4. Reversibly Switchable Enhanced Green Fluorescent Protein 2 (rsEGFP2) ............. 55 a. Generation of rsEGFP2 ............................................................................................. 55 b. Characterization of rsEGFP2 .................................................................................... 57 c. RESOLFT-type Microscopy Using rsEGFP2 ............................................................ 61 1 Table of Contents V. Discussion ........................................................................ 66 1. A Comparison of Screening Approaches Utilized for RSFP Generation .................. 67 2. Introduction of Fast, Persisting, and Reversible Switching into EGFP .................... 69 a. The Non-Linear Dependence of Light Intensity on RSFP Characteristics ................ 69 b. The Structural Basis of Switching in rsEGFP and rsEGFP2 ..................................... 70 c. The Protonation States .............................................................................................. 73 3. RESOLFT-type Microscopy Based on RSFPs ............................................................. 74 a. The Resolution of rsEGFP-RESOLFT Microscopy ................................................... 75 b. Super-Resolution Microscopy at Low Levels of Light Using rsEGFP-RESOLFT ..... 76 c. Increasing the Imaging Speed in RSFP-based RESOLFT Microscopy .................... 77 d. The Adaptability of the RESOLFT Approach to Different Experimental Needs ........ 79 4. All Optical Data Storage Approaches Using rsEGFP ................................................. 80 a. The Use of rsEGFP for Rewritable Data Storage Applications ................................. 80 b. rsEGFP Enables Diffraction-Unlimited All-Optical Writing ........................................ 82 5. Outlook ............................................................................................................................ 84 VI. Material & Methods .......................................................... 86 1. Cell and Tissue Cultures ................................................................................................ 86 a. E. coli Culturing and Transformation ......................................................................... 86 b. Mammalian Cell Culturing and Transfection ............................................................. 87 c. Preparation, Culturing, and Viral Transfection of Organtypic Hippocampal Slices ... 87 2. Cloning and Mutagenesis Strategies ............................................................................ 88 a. Plasmid Propagation from E. coli cultures ................................................................ 88 b. General Amplification Strategy for Cloning ............................................................... 88 c. Cloning of Protein Expression Plasmids ................................................................... 89 d. Cloning of Fusion Proteins ........................................................................................ 89 e. Site-Directed Mutagenesis ........................................................................................ 91 f. Error-Prone Mutagenesis .......................................................................................... 92 3. Screening strategies ...................................................................................................... 93 4. Protein Purification and Characterisation .................................................................... 93 a. Protein Expression and Purification .......................................................................... 93 b. Determination of Absorption Spectra ........................................................................ 94 c. Determination of Fluorescence Excitation and Emission Spectra ............................ 94 2 Table of Contents d. Calculation of Molecular Extinction Coefficients and Fluorescence Quantum Yield of rsEGFP and rsEGFP2 ............................................................................................... 95 e. Estimation of Single Molecule Brightness ................................................................. 95 f. Determination of Switching and Bleaching Characteristics ....................................... 96 g. Determination of Relaxation Kinetics ........................................................................ 97 h. Semi-Native Gel Electrophoresis .............................................................................. 97 i. Size Separation Chromatography ............................................................................. 98 j. Determination of Chromophor Maturation Halftime .................................................. 98 5. Sample preparation ........................................................................................................ 99 a. Preparation of Protein Polyacrylamide Layers .......................................................... 99 b. Preparing E. coli samples Expressing the rsEGFP-MreB Fusion Protein ................ 99 c. Preparing Mammalian Cell Samples for Microscopy .............................................. 100 d. Preparation of Organotypic Hippocampal Slice Cultures for Micorscopy ............... 100 6. Fluorescence Microscopy ............................................................................................ 100 a. Confocal Laser Scanning Microscopy ..................................................................... 100 b. RESOLFT Microscopy ............................................................................................. 101 c. Image Deconvolution ............................................................................................... 103 7. Data Storage Approaches ............................................................................................ 104 a. Rewritable Data Storage ........................................................................................
Load more

Recommended publications
  • Photocontrollable Fluorescent Proteins for Superresolution Imaging
    BB43CH14-Lippincott-Schwartz ARI 19 May 2014 15:54 Photocontrollable Fluorescent Proteins for Superresolution Imaging Daria M. Shcherbakova,1,2 Prabuddha Sengupta,3 Jennifer Lippincott-Schwartz,3 and Vladislav V. Verkhusha1,2 1Department of Anatomy and Structural Biology, and 2Gruss-Lipper Biophotonics Center, Albert Einstein College of Medicine, Bronx, New York 10461; email: [email protected] 3Section on Organelle Biology, Cell Biology and Metabolism Program, Eunice Kennedy Shriver National Institute of Child Health and Human Development, National Institutes of Health, Bethesda, Maryland 20892; email: [email protected] Annu. Rev. Biophys. 2014. 43:303–29 Keywords The Annual Review of Biophysics is online at PALM, RESOLFT, PAGFP, PAmCherry, EosFP biophys.annualreviews.org This article’s doi: Abstract 10.1146/annurev-biophys-051013-022836 Superresolution fluorescence microscopy permits the study of biological Copyright c 2014 by Annual Reviews. processes at scales small enough to visualize fine subcellular structures All rights reserved that are unresolvable by traditional diffraction-limited light microscopy. Many superresolution techniques, including those applicable to live cell imaging, utilize genetically encoded photocontrollable fluorescent proteins. Annu. Rev. Biophys. 2014.43:303-329. Downloaded from www.annualreviews.org The fluorescence of these proteins can be controlled by light of specific wavelengths. In this review, we discuss the biochemical and photophysi- by Yeshiva University - Albert Einstein College of Medicine on 06/06/14. For personal use only. cal properties of photocontrollable fluorescent proteins that are relevant to their use in superresolution microscopy. We then describe the recently developed photoactivatable, photoswitchable, and reversibly photoswitch- able fluorescent proteins, and we detail their particular usefulness in single- molecule localization–based and nonlinear ensemble–based superresolution techniques.
    [Show full text]
  • Two Approaches for a Simpler STED Microscope Using a Dual-Color Laser Or a Single Wavelength Ancuţa Teodora Şcheul
    Two approaches for a simpler STED microscope using a dual-color laser or a single wavelength Ancuţa Teodora Şcheul To cite this version: Ancuţa Teodora Şcheul. Two approaches for a simpler STED microscope using a dual-color laser or a single wavelength. Other [cond-mat.other]. Université de Grenoble, 2013. English. NNT : 2013GRENY040. tel-01558306 HAL Id: tel-01558306 https://tel.archives-ouvertes.fr/tel-01558306 Submitted on 7 Jul 2017 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. THESE` Pour obtenir le grade de DOCTEUR DE L’UNIVERSITE´ DE GRENOBLE Specialit´ e´ : Optique, Nanophysique Arretˆ e´ ministeriel´ : 7 aoutˆ 2006 Present´ ee´ par S¸cheul Ancut¸aTeodora These` dirigee´ par Jean-Claude Vial et codirigee´ par Irene` Wang prepar´ ee´ au sein du Laboratoire interdisciplinaire de Physique et de l’Ecole Doctorale de Physique, Grenoble Two approaches for a simpler STED microscope using a dual- color laser or a single wavelength These` soutenue publiquement le 22 Novembre 2013, devant le jury compose´ de : Dominique Bourgeois Directeur de Recherche
    [Show full text]
  • Super-Resolution Microscopy 1
    Semrock White Paper Series: Super-resolution Microscopy 1. Introduction Fluorescence microscopy has revolutionized the study of biological samples. Ever since the invention of fluorescence microscopy towards the beginning of the 20th century, significant technological advances have enabled elucidation of biological phenomenon at cellular, sub- cellular and even at molecular levels. However, the latest incarnation of the modern fluorescence microscope has led to a paradigm shift. This wave is about breaking the diffraction limit first proposed in 1873 by Ernst Abbe. The implications of this development are profound. This new technology, called super-resolution microscopy, allows for the visualization of cellular samples with a resolution similar to that of an electron microscope, yet it retains the advantages of an optical fluorescence microscope. This means it is possible to uniquely visualize desired molecular species in a cellular environment, even in three dimensions and now in live cells – all at a scale comparable to the spatial dimensions of the molecules under investigation. This article provides an overview of some of the key recent developments in super-resolution microscopy. 2. The problem So what is wrong with a conventional fluorescence microscope? To understand the answer to this question, consider a Green Fluorescence Protein (GFP) molecule that is about 3 nm in diameter and about 4 nm long. When a single GFP molecule is imaged using a 100X objective the size of the image should be 0.3 to 0.4 microns (100 times the size of the object). Yet the smallest spot that can be seen at the camera is about 25 microns. Which corresponds to an object size of about 250 nm.
    [Show full text]
  • RESOLFT Light-Sheet Microscopy
    Dissertation submitted to the Combined Faculties for the Natural Sciences and for Mathematics of the Ruperto-Carola University of Heidelberg, Germany for the degree of Doctor of Natural Sciences Put forward by Diplom-Physiker Patrick Hoyer Born in Weiden i. d. OPf. Oral examination: December 17, 2014 RESOLFT Light-sheet Microscopy Referees: Prof. Dr. Stefan W. Hell Prof. Dr. Wolfgang Petrich «φύσις κρύπτεσθαι φιλεῖ.» (“Nature loves to hide.”) Heraklit, Fragmentum, B 123. Abstract e concept of RESOLFT was introduced to break the resolution limit in fluo- rescence microscopy, which is set by the physical phenomenon of diffraction. It enables the separation of fluorophores inside a focal volume by driving re- versible optical transitions between two discernible states. e family of re- versibly switchable fluorescent proteins (RSFPs) with long-lived on- and off- states allows for RESOLFT imaging at low light levels. Up to now, RESOLFT involving RSFPs as fluorescent markers has been exclusively demonstrated to enhance the resolution in the lateral dimension. In this work, a novel RSFP- based RESOLFT microscope is presented, that, for the first time, breaks the diffraction barrier in the axial direction by switching fluorophores in the vol- ume of a light-sheet. It is realized with the optical arrangement of a selec- tive plane illumination microscope (SPIM), that illuminates only a thin sec- tion of a sample perpendicular to the detection axis and thus reduces the overall light exposure in volume recordings. e symbiotic combination of RSFP-based RESOLFT and SPIM, the so called RESOLFT-SPIM nanoscope, offers highly parallelized, fast imaging of living biological specimens with low light doses and sub-diffraction axial resolution.
    [Show full text]
  • Experimental Stochastics in High-Resolution Fluorescence
    High-Resolution Fluorescence Microscopy with Photoswitchable Fluorescent Proteins Dissertation zur Erlangung des mathematisch-naturwissenschaftlichen Doktorgrades ”Doctor rerum naturalium” der Georg-August-Universitat¨ Gottingen¨ vorgelegt von Hannes Bock aus Hamburg Gottingen,¨ 2008 . D 7 Referent: Prof. Dr. M. Munzenberg¨ Koreferent: Prof. Dr. S. W. Hell Tag der mundlichen¨ Prufung:¨ High-Resolution Fluorescence Microscopy with Photoswitchable Fluorescent Proteins Summary The diffraction limit in far-field fluorescence microscopy can be overcome by photoswitch- ing the marker molecules between a fluorescent and a non-fluorescent state. Photoswitching enables the successive generation and readout of nano-sized fluorescent areas in the sample. Subsequently, these areas can be assembled to form a super-resolution image of the speci- men. For the first time in this work, one and the same molecular switching mechanism of a reversibly switchable fluorescent protein (RSFP) was used to realize two alternative varia- tions of this general nanoscopy principle: one based on the targeted switching of ensembles of molecules and the other based on the stochastic switching of single emitters. RSFPs are of particular interest for these techniques because they allow the non-invasive study of pro- cesses in living cells and can be efficiently switched using low light intensities, thus minimiz- ing photo stress and possible photo-induced damage of the cell. Furthermore, the protein’s photoswitching properties can be improved via targeted mutagenesis. In the case of both nanoscopy techniques presented here, image acquisition could be significantly improved and accelerated as compared to related approaches. For the first time, two-color far-field fluores- cence nanoscopy based on the photoswitching of single emitters was successfully realized in biological samples.
    [Show full text]
  • Far-Field Optical Imaging and Manipulation of Individual Spins with Nanoscale Resolution
    Far-Field Optical Imaging and Manipulation of Individual Spins with Nanoscale Resolution The Harvard community has made this article openly available. Please share how this access benefits you. Your story matters Citation Maurer, P. C., J. R. Maze, P. L. Stanwix, L. Jiang, A. V. Gorshkov, A. A. Zibrov, B. Harke, et al. 2010. Far-Field Optical Imaging and Manipulation of Individual Spins with Nanoscale Resolution. Nature Physics 6, no. 11: 912–918. Published Version doi:10.1038/nphys1774 Citable link http://nrs.harvard.edu/urn-3:HUL.InstRepos:12724044 Terms of Use This article was downloaded from Harvard University’s DASH repository, and is made available under the terms and conditions applicable to Other Posted Material, as set forth at http:// nrs.harvard.edu/urn-3:HUL.InstRepos:dash.current.terms-of- use#LAA Far-field optical imaging and manipulation of individual spins with nanoscale resolution P. C. Maurer1;∗, J. R. Maze1;7;∗, P. L. Stanwix2;8;∗, L. Jiang6, A.V. Gorshkov1, A.A. Zibrov1, B. Harke3, J.S. Hodges1;4, A.S. Zibrov1, A. Yacoby1, D. Twitchen5, S.W. Hell3, R.L. Walsworth1;2, M.D. Lukin1 1Department of Physics, Harvard University, Cambridge, Massachusetts 02138 USA 2Harvard-Smithsonian Center for Astrophysics, Cambridge, Massachusetts 02138 USA 3Max Planck Institute for Biophysical Chemistry, Gottingen, Germany. 4Department of Nuclear Science and Engineering, Massachusetts Institute of Technology, Cam- bridge, Massachusetts 02139, USA 5Element Six Ltd, Ascot, Berkshire, UK. 6Institute for Quantum Information, California Institute of Technology, Pasadena, CA 91125, USA. 7Facultad de F´ısica, Pontificia Universidad Catolica´ de Chile, Casilla 306, Santiago, Chile.
    [Show full text]
  • Achromatic Light Patterning and Improved Image Reconstruction for Parallelized RESOLFT Nanoscopy
    Achromatic light patterning and improved image reconstruction for parallelized RESOLFT nanoscopy Andriy Chmyrov1,2,§†, Marcel Leutenegger1†, Tim Grotjohann1, Andreas Schönle2, Jan Keller-Findeisen1, Lars Kastrup2, Stefan Jakobs1,3, Gerald Donnert2, Steffen J. Sahl1 & Stefan W. Hell1* 1 Max Planck Institute for Biophysical Chemistry, Department of NanoBiophotonics, Am Faßberg 11, 37077 Göttingen, Germany. 2 Abberior Instruments GmbH, Hans-Adolf-Krebs-Weg 1, 37077 Göttingen, Germany. 3 University of Göttingen, Medical Faculty, Department of Neurology, Robert-Koch-Str. 40, 37075 Göttingen, Germany. § Present address: Helmholtz-Zentrum München, Institute of Biological and Medical Imaging, Ingolstädter Landstraße 1, 85764 Neuherberg, Germany. † These authors contributed equally. *Correspondence should be addressed to S.W.H. ([email protected]). Fluorescence microscopy is rapidly turning into nanoscopy. Among the various nanoscopy methods, the STED/RESOLFT super-resolution family has recently been expanded to image even large fields of view within a few seconds. This advance relies on using light patterns featuring substantial arrays of intensity minima for discerning features by switching their fluorophores between ‘on’ and ‘off’ states of fluorescence. Here we show that splitting the light with a grating and recombining it in the focal plane of the objective lens renders arrays of minima with wavelength-independent periodicity. This colour-independent creation of periodic patterns facilitates coaligned on- and off-switching and readout with combinations chosen from a range of wavelengths. Applying up to three such periodic patterns on the switchable fluorescent proteins Dreiklang and rsCherryRev1.4, we demonstrate highly parallelized, multicolour RESOLFT nanoscopy in living cells at ~60–80 nm resolution for ~100×100 μm2 fields of view.
    [Show full text]
  • The Positive Switching RSFP Padron2 Enables Live-Cell RESOLFT Nanoscopy Without Sequential Irradiation Steps
    bioRxiv preprint doi: https://doi.org/10.1101/2020.09.29.318733; this version posted September 30, 2020. The copyright holder for this preprint (which was not certified by peer review) is the author/funder, who has granted bioRxiv a license to display the preprint in perpetuity. It is made available under aCC-BY-NC-ND 4.0 International license. The Positive Switching RSFP Padron2 Enables Live-Cell RESOLFT Nanoscopy Without Sequential Irradiation Steps Timo Konen¹, Tim Grotjohann¹, Isabelle Jansen¹, Nickels Jensen¹, Stefan W. Hell¹, Stefan Jakobs¹,²* ¹Department of NanoBiophotonics, Max Planck Institute for Biophysical Chemistry, Göttingen, Germany ²Department of Neurology, University of Göttingen, Göttingen, Germany *Correspondence: [email protected] 1 bioRxiv preprint doi: https://doi.org/10.1101/2020.09.29.318733; this version posted September 30, 2020. The copyright holder for this preprint (which was not certified by peer review) is the author/funder, who has granted bioRxiv a license to display the preprint in perpetuity. It is made available under aCC-BY-NC-ND 4.0 International license. Abstract Reversibly switchable fluorescent proteins (RSFPs) can be repeatedly transferred between a fluorescent on- and a non-fluorescent off-state in response to irradiation with light of different wavelengths. Negative switching RSFPs are switched from the on- to the off-state with the same wavelength which also excites fluorescence. Positive switching RSFPs have a reversed light response where the fluorescence excitation wavelength induces the transition from the off- to the on-state. Reversible saturable optical linear (fluorescence) transitions (RESOLFT) nanoscopy utilizes these switching states to achieve diffraction-unlimited resolution, but so far has primarily relied on negative switching RSFPs by using time sequential switching schemes.
    [Show full text]
  • Three Dimensional Parallelized RESOLFT Nanoscopy for Volumetric Live Cell Imaging Andreas Bodén1, Francesca Pennacchietti1, Ilaria Testa1,†
    bioRxiv preprint doi: https://doi.org/10.1101/2020.01.09.898510; this version posted January 9, 2020. The copyright holder for this preprint (which was not certified by peer review) is the author/funder. All rights reserved. No reuse allowed without permission. Three dimensional parallelized RESOLFT nanoscopy for volumetric live cell imaging Andreas Bodén1, Francesca Pennacchietti1, Ilaria Testa1,† 1 Department of Applied Physics and Science for Life Laboratory, KTH Royal Institute of Technology, 100 44 Stockholm, Sweden; † Corresponding authors: [email protected] Abstract The volumetric architecture of organelles and molecules inside cells can only be investigated with microscopes featuring sufficiently high resolving power in all three spatial dimensions. Current methods suffer from severe limitations when applied to live cell imaging such as long recording times and/or photobleaching. By introducing a novel optical scheme to switch reversibly switchable fluorescent molecules, we demonstrate volumetric nanoscopy of living cells with resolution below 100 nm in 3D, large field of view and minimal illumination intensities (W-kW/cm2). bioRxiv preprint doi: https://doi.org/10.1101/2020.01.09.898510; this version posted January 9, 2020. The copyright holder for this preprint (which was not certified by peer review) is the author/funder. All rights reserved. No reuse allowed without permission. Optical microscopes primarily convey higher spatial information in the lateral directions due to the intrinsic principles of lens-based imaging. The advent of optical nanoscopy has demonstrated the possibility to extract isotropic axial and lateral information beyond the diffraction limit using interferometry1-3 and point spread function engineering4-6 approaches in both deterministic and single molecule stochastic switching methods.
    [Show full text]
  • Stefan W. Hell
    Nanoscopy with Focused Light Nobel Lecture, December 8, 2014 by Stefan W. Hell Max Planck Institute for Biophysical Chemistry, Department of NanoBiophotonics, Am Fassberg 11, 37077 Göttingen, Germany & German Cancer Research Center (DKFZ), Optical Nanoscopy Division, Im Neuenheimer Feld 280, 69120 Heidelberg, Germany. e are all familiar with the sayings “a picture is worth a thousand words” W and “seeing is believing.” Not only do they apply to our daily lives, but certainly also to the natural sciences. Terefore, it is probably not by chance that the historical beginning of modern natural sciences very much coincides with the invention of light microscopy. With the light microscope, mankind was able to see for the frst time that every living being consists of cells as basic units of structure and function; bacteria were discovered with the light microscope, and also mitochondria as examples of subcellular organelles. However, we learned in high school that the resolution of a light micro- scope is limited to about half the wavelength of the light in use [1–4], which typically amounts to about 200–350 nanometres (Fig. 1). If we want to see de- tails of smaller things, such as viruses, we have to resort to electron microscopy. Electron microscopy has achieved a much higher spatial resolution—ten-fold, hundred-fold or even thousand-fold higher; in fact, down to the size of a single molecule. Terefore the question comes up: Why do we bother with the light mi- croscope and its spatial resolution, now that we have the electron microscope? Te answer to this question is given in Fig.
    [Show full text]
  • Diffraction-Unlimited All-Optical Imaging and Writing with a Photochromic GFP
    ARTICLE doi:10.1038/nature10497 Diffraction-unlimited all-optical imaging and writing with a photochromic GFP Tim Grotjohann1*, Ilaria Testa1*, Marcel Leutenegger1*, Hannes Bock1, Nicolai T. Urban1, Flavie Lavoie-Cardinal1, Katrin I. Willig1, Christian Eggeling1, Stefan Jakobs1,2 & Stefan W. Hell1 Lens-based optical microscopy failed to discern fluorescent features closer than 200 nm for decades, but the recent breaking of the diffraction resolution barrier by sequentially switching the fluorescence capability of adjacent features on and off is making nanoscale imaging routine. Reported fluorescence nanoscopy variants switch these features either with intense beams at defined positions or randomly, molecule by molecule. Here we demonstrate an optical nanoscopy that records raw data images from living cells and tissues with low levels of light. This advance has been facilitated by the generation of reversibly switchable enhanced green fluorescent protein (rsEGFP), a fluorescent protein that can be reversibly photoswitched more than a thousand times. Distributions of functional rsEGFP-fusion proteins in living bacteria and mammalian cells are imaged at ,40-nanometre resolution. Dendritic spines in living brain slices are super-resolved with about a million times lower light intensities than before. The reversible switching also enables all-optical writing of features with subdiffraction size and spacings, which can be used for data storage. 22 In a fluorescence microscope, diffraction prevents (excitation) light example, d , 40 nm typically entails Im 5 100–500 MW cm (ref. 6). being focused more sharply than l/(2NA), with l being the wavelength Although intensities of this order have been demonstrated to be live- of light and NA the numerical aperture of the lens.
    [Show full text]
  • Introduction to Superresolution-Zeiss.Pdf
    11/15/12 ZEISS Microscopy Online Campus | Introduction to Superresolution Microscopy Contact Us | Carl Zeiss Education in Microscopy and Digital Imaging ZEISS Home ¦ Products ¦ Solutions ¦ Support ¦ Online Shop ¦ ZEISS International ZEISS Campus Home Interactive Tutorials Basic Microscopy Spectral Imaging Spinning Disk Microscopy Optical Sectioning Superresolution Introduction Article Quick Links Introduction Live-Cell Imaging Over the past several decades, fluorescence microscopy has become an Nearfield (NSOM) Fluorescent Proteins essential tool for examining a wide variety of biological molecules, 4Pi and InM pathways, and dynamics in living cells, tissues, and whole animals. In Microscope Light Sources RESOLFT contrast to other techniques (such as electron microscopy), fluorescence Digital Image Galleries imaging is compatible with cells that are being maintained in culture, which PSF Engineering Applications Library enables minimally invasive optical-based observation of events occurring SR-SIM on a large span of timescales. In terms of spatial resolution, several PALM & STORM Reference Library techniques including positron-emission tomography, magnetic resonance Print Version imaging, and optical coherence tomography can generate images of animal and human subjects at resolutions between 10 centimeters and 10 Search micrometers, whereas electron microscopy and scanning probe techniques feature the highest spatial resolution, often approaching the molecular and atomic levels (see Figure 1). Between these two extremes in resolving power lies optical microscopy. Aside from the benefits derived from being able to image living cells, the most significant drawback to all forms of fluorescence microscopy (including widefield, laser scanning, spinning disk, multiphoton, and total internal reflection) are the limits to spatial resolution that were first elucidated and described by Ernst Abbe in the late 1800s.
    [Show full text]