Laser Scanning Confocal Microscopy
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Second Harmonic Imaging Microscopy
170 Microsc Microanal 9(Suppl 2), 2003 DOI: 10.1017/S143192760344066X Copyright 2003 Microscopy Society of America Second Harmonic Imaging Microscopy Leslie M. Loew,* Andrew C. Millard,* Paul J. Campagnola,* William A. Mohler,* and Aaron Lewis‡ * Center for Biomedical Imaging Technology, University of Connecticut Health Center, Farmington, CT 06030-1507 USA ‡ Division of Applied Physics, Hebrew University of Jerusalem, Jerusalem 91904, Israel Second Harmonic Generation (SHG) has been developed in our laboratories as a high- resolution non-linear optical imaging microscopy (“SHIM”) for cellular membranes and intact tissues. SHG is a non-linear process that produces a frequency doubling of the intense laser field impinging on a material with a high second order susceptibility. It shares many of the advantageous features for microscopy of another more established non-linear optical technique: two-photon excited fluorescence (TPEF). Both are capable of optical sectioning to produce 3D images of thick specimens and both result in less photodamage to living tissue than confocal microscopy. SHG is complementary to TPEF in that it uses a different contrast mechanism and is most easily detected in the transmitted light optical path. It also does not arise via photon emission from molecular excited states, as do both 1- and 2-photon excited fluorescence. SHG of intrinsic highly ordered biological structures such as collagen has been known for some time but only recently has the full potential of high resolution 3D SHIM been demonstrated on live cells and tissues. For example, Figure 1 shows SHIM from microtubules in a living organism, C. elegans. The images were obtained from a transgenic nematode that expresses a ß-tubulin-green fluorescent protein fusion and Figure 1 also shows the TPEF image from this molecule for comparison. -
Multiphoton Microscopy
Living up to Life Multiphoton Microscopy 1 Jablonski Diagram: Living up to Life Nonlinear Optical Microscopy F.- Helmchen, W. Denk, Deep tissue two-photon microscopy, Nat. Methods 2, 932-940 2 Typical Samples – Living up to Life Small Dimensions & Highly Scattering • Somata 10-30 µm • Dendrites 1-5 µm • Spines ~0.5 µm • Axons 1-2 µm ls ~ 50-100 µm (@ 630 nm) ls ~ 200 µm (@ 800 nm) T. Nevian Institute of Physiology University of Bern, Switzerland F.- Helmchen, W. Denk Deep tissue two-photon microscopy. Nat. Methods 2, 932-940 3 Why Multiphoton microscopy? Living up to Life • Today main challenge: To go deeper into samples for improved studies of cells, organs or tissues, live animals Less photodamage, i.e. less bleaching and phototoxicity • Why is it possible? Due to the reduced absorption and scattering of the excitation light 4 The depth limit Living up to Life • Achievable depth: ~ 300 – 600 µm • Maximum imaging depth depends on: – Available laser power – Scattering mean-free-path – Tissue properties • Density properties • Microvasculature organization • Cell-body arrangement • Collagen / myelin content – Specimen age – Collection efficiency Acute mouse brain sections containing YFP neurons,maximum projection, Z stack: 233 m Courtesy: Dr Feng Zhang, Deisseroth laboratory, Stanford University, USA Page 5 What is Two‐Photon Microscopy? Living up to Life A 3-dimensional imaging technique in which 2 photons are used to excite fluorescence emission exciting photon emitted photon S1 Simultaneous absorption of 2 longer wavelength photons to -
Adaptive Optics in Microscopy
Downloaded from http://rsta.royalsocietypublishing.org/ on February 3, 2015 Phil. Trans. R. Soc. A (2007) 365, 2829–2843 doi:10.1098/rsta.2007.0013 Published online 13 September 2007 Adaptive optics in microscopy BY MARTIN J. BOOTH* Department of Engineering Science, University of Oxford, Parks Road, Oxford OX1 3PJ, UK The imaging properties of optical microscopes are often compromised by aberrations that reduce image resolution and contrast. Adaptive optics technology has been employed in various systems to correct these aberrations and restore performance. This has required various departures from the traditional adaptive optics schemes that are used in astronomy. This review discusses the sources of aberrations, their effects and their correction with adaptive optics, particularly in confocal and two-photon microscopes. Different methods of wavefront sensing, indirect aberration measurement and aberration correction devices are discussed. Applications of adaptive optics in the related areas of optical data storage, optical tweezers and micro/nanofabrication are also reviewed. Keywords: adaptive optics; aberrations; confocal microscopy; multiphoton microscopy; optical data storage; optical tweezers 1. Introduction Optical microscopes are essential tools in many scientific fields. In the life sciences, they are widely used for the visualization of cellular structures and sub- cellular processes. Confocal and multiphoton microscopes are particularly important in this respect as they produce three-dimensional images of volumetric objects. However, the resolution of these microscopes is often adversely affected by the optical properties of the specimen itself. Spatial variations in the refractive index of the specimen introduce optical aberrations that compromise image quality. This is a particular problem when imaging deep into thick biological specimens. -
Fv1000 Fluoview
Confocal Laser Scanning Biological Microscope FV1000 FLUOVIEW FLUOVIEW—Always Evolving FLUOVIEW–—From Olympus is Open FLUOVIEW—More Advanced than Ever The Olympus FLUOVIEW FV1000 confocal laser scanning microscope delivers efficient and reliable performance together with the high resolution required for multi-dimensional observation of cell and tissue morphology, and precise molecular localization. The FV1000 incorporates the industry’s first dedicated laser light stimulation scanner to achieve simultaneous targeted laser stimulation and imaging for real-time visualization of rapid cell responses. The FV1000 also measures diffusion coefficients of intracellular molecules, quantifying molecular kinetics. Quite simply, the FLUOVIEW FV1000 represents a new plateau, bringing “imaging to analysis.” Olympus continues to drive forward the development of FLUOVIEW microscopes, using input from researchers to meet their evolving demands and bringing “imaging to analysis.” Quality Performance with Innovative Design FV10i 1 Imaging to Analysis ing up New Worlds From Imaging to Analysis FV1000 Advanced Deeper Imaging with High Resolution FV1000MPE 2 Advanced FLUOVIEW Systems Enhance the Power of Your Research Superb Optical Systems Set the Standard for Accuracy and Sensitivity. Two types of detectors deliver enhanced accuracy and sensitivity, and are paired with a new objective with low chromatic aberration, to deliver even better precision for colocalization analysis. These optical advances boost the overall system capabilities and raise performance to a new level. Imaging, Stimulation and Measurement— Advanced Analytical Methods for Quantification. Now equipped to measure the diffusion coefficients of intracellular molecules, for quantification of the dynamic interactions of molecules inside live cell. FLUOVIEW opens up new worlds of measurement. Evolving Systems Meet the Demands of Your Application. -
Two-Photon Excitation Fluorescence Microscopy
P1: FhN/ftt P2: FhN July 10, 2000 11:18 Annual Reviews AR106-15 Annu. Rev. Biomed. Eng. 2000. 02:399–429 Copyright c 2000 by Annual Reviews. All rights reserved TWO-PHOTON EXCITATION FLUORESCENCE MICROSCOPY PeterT.C.So1,ChenY.Dong1, Barry R. Masters2, and Keith M. Berland3 1Department of Mechanical Engineering, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139; e-mail: [email protected] 2Department of Ophthalmology, University of Bern, Bern, Switzerland 3Department of Physics, Emory University, Atlanta, Georgia 30322 Key Words multiphoton, fluorescence spectroscopy, single molecule, functional imaging, tissue imaging ■ Abstract Two-photon fluorescence microscopy is one of the most important re- cent inventions in biological imaging. This technology enables noninvasive study of biological specimens in three dimensions with submicrometer resolution. Two-photon excitation of fluorophores results from the simultaneous absorption of two photons. This excitation process has a number of unique advantages, such as reduced specimen photodamage and enhanced penetration depth. It also produces higher-contrast im- ages and is a novel method to trigger localized photochemical reactions. Two-photon microscopy continues to find an increasing number of applications in biology and medicine. CONTENTS INTRODUCTION ................................................ 400 HISTORICAL REVIEW OF TWO-PHOTON MICROSCOPY TECHNOLOGY ...401 BASIC PRINCIPLES OF TWO-PHOTON MICROSCOPY ..................402 Physical Basis for Two-Photon Excitation ............................ -
Confocal Microscopy
Confocal microscopy Chapter in Handbook of Comprehensive Biophysics ( in press 2011) Elsevier Brad Amos MRC Laboratory of Molecular Biology, Hills Road, Cambridge CB2 0QH UK e-mail [email protected] Gail McConnell University of Strathclyde , Centre for Biophotonics 161 Cathedral Street , Glasgow G4 0RE UK [email protected] Tony Wilson Dept. of Engineering Science, University of Oxford, Parks Road, Oxford, OX1 3PJ, UK. eMail: [email protected] 1 Introduction A confocal microscope is one in which the illumination is confined to a small volume in the specimen, the detection is confined to the same volume and the image is built up by scanning this volume over the specimen, either by moving the beam of light over the specimen or by displacing the specimen relative to a stationary beam. The chief advantage of this type of microscope is that it gives a greatly enhanced discrimination of depth relative to conventional microscopes. Commercial systems appeared in the 1980s and, despite their high cost, the world market for them is probably between 500 and 1000 instruments per annum, mainly because of their use in biomedical research in conjunction with fluorescent labelling methods. There are many books and review articles on this subject ( e.g. Pawley ( 2006) , Matsumoto( 2002), Wilson (1990) ). The purpose of this chapter is to provide an introduction to optical and engineering aspects that may be o f interest to biomedical users of confocal microscopy. Flying-spot Microscopes A confocal microscope is a special type of ‘flying spot’ microscope. Flying spot systems were developed in the 1950s by combining conventional microscopes with electronics from TV and military equipment. -
Imaging with Second-Harmonic Generation Nanoparticles
1 Imaging with Second-Harmonic Generation Nanoparticles Thesis by Chia-Lung Hsieh In Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy California Institute of Technology Pasadena, California 2011 (Defended March 16, 2011) ii © 2011 Chia-Lung Hsieh All Rights Reserved iii Publications contained within this thesis: 1. C. L. Hsieh, R. Grange, Y. Pu, and D. Psaltis, "Three-dimensional harmonic holographic microcopy using nanoparticles as probes for cell imaging," Opt. Express 17, 2880–2891 (2009). 2. C. L. Hsieh, R. Grange, Y. Pu, and D. Psaltis, "Bioconjugation of barium titanate nanocrystals with immunoglobulin G antibody for second harmonic radiation imaging probes," Biomaterials 31, 2272–2277 (2010). 3. C. L. Hsieh, Y. Pu, R. Grange, and D. Psaltis, "Second harmonic generation from nanocrystals under linearly and circularly polarized excitations," Opt. Express 18, 11917–11932 (2010). 4. C. L. Hsieh, Y. Pu, R. Grange, and D. Psaltis, "Digital phase conjugation of second harmonic radiation emitted by nanoparticles in turbid media," Opt. Express 18, 12283–12290 (2010). 5. C. L. Hsieh, Y. Pu, R. Grange, G. Laporte, and D. Psaltis, "Imaging through turbid layers by scanning the phase conjugated second harmonic radiation from a nanoparticle," Opt. Express 18, 20723–20731 (2010). iv Acknowledgements During my five-year Ph.D. studies, I have thought a lot about science and life, but I have never thought of the moment of writing the acknowledgements of my thesis. At this moment, after finishing writing six chapters of my thesis, I realize the acknowledgment is probably one of the most difficult parts for me to complete. -
Super-Resolution Imaging by Dielectric Superlenses: Tio2 Metamaterial Superlens Versus Batio3 Superlens
hv photonics Article Super-Resolution Imaging by Dielectric Superlenses: TiO2 Metamaterial Superlens versus BaTiO3 Superlens Rakesh Dhama, Bing Yan, Cristiano Palego and Zengbo Wang * School of Computer Science and Electronic Engineering, Bangor University, Bangor LL57 1UT, UK; [email protected] (R.D.); [email protected] (B.Y.); [email protected] (C.P.) * Correspondence: [email protected] Abstract: All-dielectric superlens made from micro and nano particles has emerged as a simple yet effective solution to label-free, super-resolution imaging. High-index BaTiO3 Glass (BTG) mi- crospheres are among the most widely used dielectric superlenses today but could potentially be replaced by a new class of TiO2 metamaterial (meta-TiO2) superlens made of TiO2 nanoparticles. In this work, we designed and fabricated TiO2 metamaterial superlens in full-sphere shape for the first time, which resembles BTG microsphere in terms of the physical shape, size, and effective refractive index. Super-resolution imaging performances were compared using the same sample, lighting, and imaging settings. The results show that TiO2 meta-superlens performs consistently better over BTG superlens in terms of imaging contrast, clarity, field of view, and resolution, which was further supported by theoretical simulation. This opens new possibilities in developing more powerful, robust, and reliable super-resolution lens and imaging systems. Keywords: super-resolution imaging; dielectric superlens; label-free imaging; titanium dioxide Citation: Dhama, R.; Yan, B.; Palego, 1. Introduction C.; Wang, Z. Super-Resolution The optical microscope is the most common imaging tool known for its simple de- Imaging by Dielectric Superlenses: sign, low cost, and great flexibility. -
Contrast Enhancement for Topographic Imaging in Confocal Laser Scanning Microscopy
applied sciences Article Contrast Enhancement for Topographic Imaging in Confocal Laser Scanning Microscopy Lena Schnitzler *,†, Markus Finkeldey †, Martin R. Hofmann and Nils C. Gerhardt Photonics and Terahertz Technology, Ruhr University Bochum, 44780 Bochum, Germany * Correspondence: [email protected] † These authors contributed equally to this work. Received: 26 June 2019; Accepted: 29 July 2019; Published: 31 July 2019 Featured Application: The method for contrast enhancement presented in this work, can be used to increase the image contrast of topographic structures. It might be an essential tool for non-destructive testing in the quality management of microcontroller production, in the processing of semiconductors or in the developement and characterization of MEMs. Even structures with low height variance can be observed. Abstract: The influence of the axial pinhole position in a confocal microscope in terms of the contrast of the image is analyzed. The pinhole displacement method is introduced which allows to increase the contrast for topographic imaging. To demonstrate this approach, the simulated data of a confocal setup as well as experimental data is shown. The simulated data is verified experimentally by a custom stage scanning reflective microscopy setup using a semiconductor test target with low contrast structures of sizes between 200 nm and 500 nm. With the introduced technique, we are able to achieve a contrast enhancement of up to 80% without loosing diffraction limited resolution. We do not add additional components to the setup, thus our concept is applicable for all types of confocal microscopes. Furthermore, we show the application of the contrast enhancement in imaging integrated circuits. Keywords: microscopy; confocal microscopy; contrast enhancement 1. -
Development of Optical Hyperlens for Imaging Below the Diffraction Limit
Development of optical hyperlens for imaging below the diffraction limit Hyesog Lee, Zhaowei Liu, Yi Xiong, Cheng Sun and Xiang Zhang* 5130 Etcheverry Hall, NSF Nanoscale Science and Engineering Center (NSEC), University of California, Berkeley, CA 94720 *Corresponding author: [email protected] http://xlab.me.berkeley.edu Abstract: We report here the design, fabrication and characterization of optical hyperlens that can image sub-diffraction-limited objects in the far field. The hyperlens is based on an artificial anisotropic metamaterial with carefully designed hyperbolic dispersion. We successfully designed and fabricated such a metamaterial hyperlens composed of curved silver/alumina multilayers. Experimental results demonstrate far-field imaging with resolution down to 125nm at 365nm working wavelength which is below the diffraction limit. ©2007 Optical Society of America OCIS codes: (110 0180) Microscopy; (220.4241) Optical design and fabrication: Nanostructure fabrication References and links 1. E. Abbe, Arch. Mikroskop. Anat. 9, 413 (1873) 2. E. Betzig, J. K. Trautman, T. D. Harris, J. S. Weiner and R. L. Kostelak, “Breaking the diffraction barrier – optical microscopy on a nanometric scale,” Science 251, 1468-1470 (1991) 3. S. W. Hell, “Toward Fluorescence nanoscopy,” Nat. Biotechnol. 21, 1347-1355 (2003) 4. M. G. L. Gustafsson, “Nonlinear structured-illumination microscopy: Wide-field fluorescence imaging with theoretically unlimited resolution,” P. Natl. Acad. Sci. 102, 13081-13086 (2005) 5. J. B. Pendry, “Negative refraction makes a perfect lens,” Phys. Rev. Lett. 85, 3966-3969 (2000) 6. N. Fang, H. Lee, C. Sun and X. Zhang, “Sub-Diffraction-Limited Optical Imaging with a Silver Superlens” Science 308, 534-537 (2005) 7. -
Development of the Optical Microscope
White Paper Development of the Optical Microscope By Peter Banks Ph.D., Scientific Director, Applications Dept., BioTek Instruments, Inc. Products: Cytation 5 Cell Imaging Multi-Mode Reader An Optical Microscope commonly found in schools and universities all over the world. Table of Contents Ptolemy and Light Refraction --------------------------------------------------------------------------------------------- 2 Islamic Polymaths and Optics -------------------------------------------------------------------------------------------- 2 The First Microscope ------------------------------------------------------------------------------------------------------- 2 Hook and Micrographia --------------------------------------------------------------------------------------------------- 2 Van Leeuwenhoek and Animalcules ------------------------------------------------------------------------------------ 5 Abbe Limit -------------------------------------------------------------------------------------------------------------------- 6 Zernicke and Phase Contrast --------------------------------------------------------------------------------------------- 7 Fluorescence Microscopy ------------------------------------------------------------------------------------------------- 7 Confocal Microscopy ------------------------------------------------------------------------------------------------------- 8 BioTek Instruments, Inc. Digital Microscopy ---------------------------------------------------------------------------------------------------------- -
Optical Tweezers and Confocal Microscopy for Simultaneous Three-Dimensional Manipulation and Imaging in Concentrated Colloidal Dispersions Dirk L
REVIEW OF SCIENTIFIC INSTRUMENTS VOLUME 75, NUMBER 9 SEPTEMBER 2004 Optical tweezers and confocal microscopy for simultaneous three-dimensional manipulation and imaging in concentrated colloidal dispersions Dirk L. J. Vossena) and Astrid van der Horst FOM Institute for Atomic and Molecular Physics, Kruislaan 407, 1098 SJ Amsterdam, and Soft Condensed Matter, Debye Institute, Utrecht University, Princetonplein 5, 3584 CC Utrecht, The Netherlands Marileen Dogterom FOM Institute for Atomic and Molecular Physics, Kruislaan 407, 1098 SJ Amsterdam, The Netherlands Alfons van Blaaderenb) FOM Institute for Atomic and Molecular Physics, Kruislaan 407, 1098 SJ Amsterdam, and Soft Condensed Matter, Debye Institute, Utrecht University, Princetonplein 5, 3584 CC Utrecht, The Netherlands (Received 25 February 2004; accepted 10 June 2004; published 14 September 2004) A setup is described for simultaneous three-dimensional manipulation and imaging inside a concentrated colloidal dispersion using (time-shared) optical tweezers and confocal microscopy. The use of two microscope objectives, one above and one below the sample, enables imaging to be completely decoupled from trapping. The instrument can be used in different trapping (inverted, upright, and counterpropagating) and imaging modes. Optical tweezers arrays, dynamically changeable and capable of trapping several hundreds of micrometer-sized particles, were created using acousto-optic deflectors. Several schemes are demonstrated to trap three-dimensional colloidal structures with optical tweezers. One combined a Pockels cell and polarizing beam splitters to create two trapping planes at different depths in the sample, in which the optical traps could be manipulated independently. Optical tweezers were used to manipulate collections of particles inside concentrated colloidal dispersions, allowing control over colloidal crystallization and melting.