T H E J O U R N A L O F C E L L B I O L O G Y
|
|
- Della Malone
- 6 years ago
- Views:
Transcription
1 T H E J O U R N A L O F C E L L B I O L O G Y Supplemental material Sikirzhytski et al., Figure S1. Behavior and organization of K-fibers in PtK 2 cells during metaphase. (A) Kymograms of individual K-fibers with photobleached marks (PM). K denotes position of the kinetochore. Notice that the bleached mark moves poleward continuously and monotonously as expected for poleward flux of MT subunits. The rate of flux varies significantly among individual K-fibers (0.5, 0.8, and 1.1 µm/min in these examples). (B) The rate of flux does not change during transition from metaphase to anaphase. AO marks anaphase onset. (C) Reorientation of the K-fiber stub toward the opposite spindle pole. Selected frames from a time-lapse recording are similar to Fig. 1 A. In this example, the distal end of a stub created by laser severing of a K-fiber (arrows) makes contact with a MT connected to the opposite spindle pole (29 s). Poleward gliding of the stub alongside this MT transports the stub with the attached kinetochore poleward, ultimately converting a proper amphitelic attachment into a syntelic one. The chromosome subsequently moves poleward and becomes monooriented. Time is in seconds from the time of the laser burst. (D and D ) Minus end of laser-severed K-fibers are decorated with NuMA. (D) Overview (maximal-intensity projection) of a cell with severed K-fiber. (D ) Through-focus series (200-nm steps) for the area boxed in D. Notice accumulation of NuMA at the severed end of the fiber. A single MT appears to interact with the stub. Notice that the distance between sister kinetochores (K1 and K2) is 1.9 µm. S1
2 Figure S2. Behavior of laser-severed K-fibers in rounded and flattened PtK 2 cells during anaphase. (A) K-fiber stubs are transported poleward during anaphase. Similar to Fig. 1 B; however, in this example, the severed K-fiber reaches the pole in a single rapid movement. (A ) Kymogram analysis demonstrates that the K-fiber stub remains motionless for 10 s and then moves poleward at 6 µm/min. Time is in seconds from the time of the laser burst. X marks the laser beam. See Video 5 for the full record. (B) Behavior of chromosomes with severed K-fibers is similar in flattened and rounded cells. In this example, a K-fiber is severed 1 µm from the kinetochore (X) in a PtK 2 cell flattened to 4.5 µm (see Materials and methods). The K-fiber fragment attached to the spindle pole depolymerizes rapidly (blue arrows), whereas the distal end of the stub attached to the chromosome connects to neighboring MTs (yellow arrows). Notice that the initial length of the K-fiber stub is 1 µm but it gradually elongates during the recording. The stub also appears to split into two fibers that maintain multiple connections with neighboring MTs (66 and 107 s). The cell initiates anaphase at 230 s and the chromatid with severed K-fiber is rapidly transported poleward. Notice that it reaches the pole significantly faster than the other chromosomes (arrows in 380 and 444 s). Time in seconds from the laser burst. See Video 6 for the full record. S2
3 Figure S3. Mitosis in RPE1 cells flattened to 3 µm. (A and A ) The spatial distribution of kinetochores and centrosomes during metaphase in rounded (A) versus flattened (A ) cells. Notice that the width and depth of the rounded spindle are similar. Extensive Z-series are necessary for the reliable tracking of kinetochores. The spindle in a cell flattened to 3 µm is longer and wider; however, the chromosomes are properly congressed. The spindle is parallel to the coverslip and the movements of individual chromosomes occur primarily in a single focal plane. (B) No abnormalities are apparent at the earlier stages of mitosis in flattened cells (see cells 1, 2, and 3). However, mitosis in flattened cells is prolonged and spindle poles often fragment at later stages, resulting in multipolar anaphase and cytokinesis (cells 1 and 2). Time in h:min. S3
4 Figure S4. K-fibers lacking attachment to the spindle poles visualized in cold-treated cells. (A) A metaphase RPE1 cell exposed to 0 C for 2 min before fixation. Only cold-stable MTs remain. Multiple short K-fibers forming side attachments to K-fibers of other chromosomes are prominent (arrows). Local maximal-intensity projections (two to four Z-sections) are shown for the boxed areas. (B) Similar to A but the cell is in anaphase. Red, MTs (also shown in grayscale); green, kinetochores (CenpA-GFP) and centrioles (Centrin-GFP); blue, chromosomes (DNA). (C) Similar to A but a metaphase U2OS cell. Multiple short K-fibers forming side attachments to K-fibers of other chromosomes are prominent (arrows). Red, MTs ( -tubulin; also shown in grayscale); green, kinetochores (CenpB-GFP); blue, chromosomes (DNA). S4
5 Figure S5. NuMA concentrates at the ends of K-fibers that lack attachment to the spindle poles. (A) The distribution of the dynein-interacting protein NuMA in cold-treated RPE1 cells (0 C for 2 min) during metaphase. NuMA is highly concentrated at the minus ends of K-fibers attached to spindle poles and is present at a significantly lower concentration in small patches throughout the spindle (A ). Mild accumulation of NuMA is seen at the minus ends of short K-fibers that do not reach the poles. (B) The association of NuMA with a short K-fiber in PtK 2 cell during anaphase. Notice that the short fiber is masked in the total maximal-intensity projection (arrow). (B ) However, it can be detected in the projection of a 1-µm-thick volume. (B ) Premature termination of the K-fiber and the association of the minus end with NuMA becomes apparent in the series of individual focal planes separated by 200-nm steps. S5
6 Video 1. Typical behavior of laser-severed K-fibers during metaphase. Laser-severed K-fibers in PtK 2 cells expressing GFP -tubulin were analyzed by time-lapse spinning-disc confocal (Yokogawa Electric Corporation) microscopy using a microscope (TE-2000E PFS; Nikon). Selected frames from this recording are shown in Fig. 1 A. 0.5-s intervals (49.5 s), 108-nm pixels, 100 NA 1.4 objective. Time in seconds. 0 corresponds to laser irradiation. Video 2. Reorientation of laser-severed K-fiber. Laser-severed K-fibers in PtK 2 cells expressing GFP -tubulin were analyzed by time-lapse confocal microscopy using a microscope (TE-2000E PFS; Nikon). Selected frames from this recording are shown in Fig. S1 C. 1-s intervals (599 s), 108-nm pixels, 100 NA 1.4 objective. Time in seconds. 0 corresponds to laser irradiation. Video 3. Laser operation and live-cell recording followed by fixation and subsequent correlative LM/EM analysis. Lasersevered K-fibers in PtK 2 cells expressing GFP -tubulin were analyzed by time-lapse confocal microscopy using a microscope (TE-2000E PFS; Nikon). X marks the laser beam. Selected frames from this recording are shown in Fig. 1 B. 0.5-s intervals (38.5 s), 108-nm pixels, 100 NA 1.4 objective. Time in seconds. 0 corresponds to laser irradiation. Video 4. Typical behavior of laser-severed K-fibers during anaphase. Laser-severed K-fibers in PtK 2 cells expressing GFP -tubulin were analyzed by time-lapse confocal microscopy using a microscope (TE-2000E PFS; Nikon). Selected frames from this recording are shown in Fig. 1 B. 0.5-s intervals (49.5 s), 108-nm pixels, 100 NA 1.4 objective. Time in seconds. 0 corresponds to laser irradiation. Video 5. Extended rapid poleward movement of laser-severed K-fiber during anaphase. Laser-severed K-fibers in PtK 2 cells expressing GFP -tubulin were analyzed by time-lapse confocal microscopy using a microscope (TE-2000E PFS; Nikon). Selected frames from this recording are shown in Fig. S1 C. 1-s intervals (32 s), 108-nm pixels, 100 NA 1.4 objective. Time in seconds. 0 corresponds to laser irradiation. S6
7 Video 6. Typical behavior of laser-severed K-fibers in a flattened cell. Laser-severed K-fibers in PtK 2 cells expressing GFP -tubulin were analyzed by time-lapse confocal microscopy using a microscope (TE-2000E PFS; Nikon). Selected frames from this recording are shown in Fig. S2 D. 1-s intervals (450 s), 108-nm pixels, 100 NA 1.4 objective. Time in seconds. Laser irradiation immediately after time 0. Flattened PtK 2 cells were obtained by placing a coverslip with microfabricated feet of known height (3 µm) on top of the coverslip with the growing cells. Video 7. Comparison of Pacman versus fiber transport mechanisms of chromosome segregation. Laser-severed K-fibers in PtK 2 cells expressing GFP -tubulin (Takara Bio Inc.) were analyzed by time-lapse confocal microscopy using a microscope (TE-2000E PFS; Nikon). Selected frames from this recording are shown in Fig. 2 (C and D). 1-s intervals (54 s), 108-nm pixels, 100 NA 1.4 objective. Time in seconds. Laser irradiation shortly before time 0. Video 8. Walk-through array-tomography reconstruction of metaphase spindle in an RPE1 cell. Phase-contrast (left) and fluorescence (right) images obtained from serial 200-nm-thin Lowicryl sections. (right) Arrows denote the minus ends of K-fibers that lack direct attachment to the spindle poles. Selected images from this reconstruction are shown in Fig. 5 (A and B). Images recorded on a Revolution spinning-disc confocal system (Andor Technology) at 55-nm pixel size. 100 NA 1.4 objective lens (Nikon). Video 9. Image transformation used for the generation of kymograms of cells with labeled centrosomes and kinetochores. Time-lapse confocal microscopy using a microscope (TE-2000E PFS; Nikon). The panels are maximal intensity projections of 3D volumes recorded at 5-s intervals before (raw) and after (aligned) each volume was rotated and shifted to make the mother centriole in the left centrosome pseudo-stationary and to fix the axis of spindle in the horizontal position. An RPE1 cell expressing CenpA-GFP and centrin-gfp. Time in min:s. 5-s intervals (320 s), 108-nm pixels, 100 NA 1.4 objective, and 500-nm Z-steps. Video 10. Image transformation used for the generation of kymograms in recordings with labeled MTs. Laser-severed K-fibers in PtK 2 cells expressing GFP -tubulin were analyzed by time-lapse confocal microscopy using a microscope (TE-2000E PFS; Nikon). Each frame was rotated and shifted to make the plus end of the K-fiber stub (kinetochore) pseudo-stationary and fix the orientation of the stub in the horizontal position. Time in min:s. 1-s intervals (100 s), 108-nm pixels, 100 NA 1.4 objective. Table S1 shows the results of laser microsurgery experiments. S7
T H E J O U R N A L O F C E L L B I O L O G Y
T H E J O U R N A L O F C E L L B I O L O G Y Supplemental material Gusnowski and Srayko, http://www.jcb.org/cgi/content/full/jcb.201103128/dc1 Figure S1. EB1-GFP velocities from the centrosomes. (A) Mean
More informationSupplementary Information. Stochastic Optical Reconstruction Microscopy Imaging of Microtubule Arrays in Intact Arabidopsis thaliana Seedling Roots
Supplementary Information Stochastic Optical Reconstruction Microscopy Imaging of Microtubule Arrays in Intact Arabidopsis thaliana Seedling Roots Bin Dong 1,, Xiaochen Yang 2,, Shaobin Zhu 1, Diane C.
More information3D light microscopy techniques
3D light microscopy techniques The image of a point is a 3D feature In-focus image Out-of-focus image The image of a point is not a point Point Spread Function (PSF) 1D imaging 2D imaging 3D imaging Resolution
More informationRapid Adaptive Optical Recovery of Optimal Resolution over Large Volumes
SUPPLEMENTARY MATERIAL Rapid Adaptive Optical Recovery of Optimal Resolution over Large Volumes Kai Wang, Dan Milkie, Ankur Saxena, Peter Engerer, Thomas Misgeld, Marianne E. Bronner, Jeff Mumm, and Eric
More informationWhy and How? Daniel Gitler Dept. of Physiology Ben-Gurion University of the Negev. Microscopy course, Michmoret Dec 2005
Why and How? Daniel Gitler Dept. of Physiology Ben-Gurion University of the Negev Why use confocal microscopy? Principles of the laser scanning confocal microscope. Image resolution. Manipulating the
More informationResolution. Diffraction from apertures limits resolution. Rayleigh criterion θ Rayleigh = 1.22 λ/d 1 peak at 2 nd minimum. θ f D
Microscopy Outline 1. Resolution and Simple Optical Microscope 2. Contrast enhancement: Dark field, Fluorescence (Chelsea & Peter), Phase Contrast, DIC 3. Newer Methods: Scanning Tunneling microscopy (STM),
More informationPoint Spread Function. Confocal Laser Scanning Microscopy. Confocal Aperture. Optical aberrations. Alternative Scanning Microscopy
Bi177 Lecture 5 Adding the Third Dimension Wide-field Imaging Point Spread Function Deconvolution Confocal Laser Scanning Microscopy Confocal Aperture Optical aberrations Alternative Scanning Microscopy
More informationDevelopment of a High-speed Super-resolution Confocal Scanner
Development of a High-speed Super-resolution Confocal Scanner Takuya Azuma *1 Takayuki Kei *1 Super-resolution microscopy techniques that overcome the spatial resolution limit of conventional light microscopy
More informationNikon. King s College London. Imaging Centre. N-SIM guide NIKON IMAGING KING S COLLEGE LONDON
N-SIM guide NIKON IMAGING CENTRE @ KING S COLLEGE LONDON Starting-up / Shut-down The NSIM hardware is calibrated after system warm-up occurs. It is recommended that you turn-on the system for at least
More informationThings to check before start-up.
Byeong Cha Page 1 11/24/2009 Manual for Leica SP2 Confocal Microscope Enter you name, the date, the time, and the account number in the user log book. Things to check before start-up. Make sure that your
More informationLight Microscopy. Upon completion of this lecture, the student should be able to:
Light Light microscopy is based on the interaction of light and tissue components and can be used to study tissue features. Upon completion of this lecture, the student should be able to: 1- Explain the
More informationT H E J O U R N A L O F C E L L B I O L O G Y
Supplemental material Parton et al., http://www.jcb.org/cgi/content/full/jcb.201103160/dc1 T H E J O U R N A L O F C E L L B I O L O G Y Figure S1. MTs in the oocyte lack posttranslational modifications
More informationNikon Instruments Europe
Nikon Instruments Europe Recommendations for N-SIM sample preparation and image reconstruction Dear customer, We hope you find the following guidelines useful in order to get the best performance out of
More information3D light microscopy techniques
3D light microscopy techniques The image of a point is a 3D feature In-focus image Out-of-focus image The image of a point is not a point Point Spread Function (PSF) 1D imaging 1 1 2! NA = 0.5! NA 2D imaging
More informationConfocal Microscopy. Kristin Jensen
Confocal Microscopy Kristin Jensen 17.11.05 References Cell Biological Applications of Confocal Microscopy, Brian Matsumoto, chapter 1 Studying protein dynamics in living cells,, Jennifer Lippincott-Schwartz
More information3. are adherent cells (ie. cells in suspension are too far away from the coverslip)
Before you begin, make sure your sample... 1. is seeded on #1.5 coverglass (thickness = 0.17) 2. is an aqueous solution (ie. fixed samples mounted on a slide will not work - not enough difference in refractive
More informationMultifluorescence The Crosstalk Problem and Its Solution
Multifluorescence The Crosstalk Problem and Its Solution If a specimen is labeled with more than one fluorochrome, each image channel should only show the emission signal of one of them. If, in a specimen
More informationSupporting Information
Supporting Information Copyright Wiley-VCH Verlag GmbH & Co. KGaA, 69451 Weinheim, 2014 Two-Color RESOLFT Nanoscopy with Green and Red Fluorescent Photochromic Proteins** Flavie Lavoie-Cardinal, [a] Nickels
More informationSuper-resolution video microscopy of live cells by structured illumination
nature methods Super-resolution video microscopy of live cells by structured illumination Peter Kner, Bryant B Chhun, Eric R Griffis, Lukman Winoto & Mats G L Gustafsson Supplementary figures and text:
More informationDifferential Interference Contrast (DIC) Verses Dark Field and Phase Contrast Microscopy. E. D. Salmon University of North Carolina at Chapel Hill
Differential Interference Contrast (DIC) Verses Dark Field and Phase Contrast Microscopy E. D. Salmon University of North Carolina at Chapel Hill How Does Contrast in DIC Differ from Phase and Pol? n e
More informationSeeing in Biology. Resolving Power of Optical Devices. Bio 101 Laboratory 2. Microscope Intro to Cell Cycle Mitosis
Bio 101 Laboratory 2 Microscope Intro to Cell Cycle Mitosis 1 Seeing in Biology There are many different tools that biologists/anatomists can use to see biological samples at high resolution. Some include:
More informationConfocal Microscopy. (Increasing contrast and resolu6on using op6cal sec6oning) Lecture 7. November 2017
Confocal Microscopy (Increasing contrast and resolu6on using op6cal sec6oning) Lecture 7 November 2017 3 Flavours of Microscope Confocal Laser Scanning Problem: Out of Focus Light Spinning disc 2-Photon
More informationMore fancy SPIM, Even fancier SPIM
More fancy SPIM, Even fancier SPIM Last class Light sheet microscopy Fancy SPIM (ispim, dspim, etc ) This class Multi camera SPIM SIM SPIM Bessels d x,y = λ em 2 NA d z = 2 NA λ ex + n(1 cosθ λ em 1 IsoView
More informationAkinori Mitani and Geoff Weiner BGGN 266 Spring 2013 Non-linear optics final report. Introduction and Background
Akinori Mitani and Geoff Weiner BGGN 266 Spring 2013 Non-linear optics final report Introduction and Background Two-photon microscopy is a type of fluorescence microscopy using two-photon excitation. It
More informationHigh-resolution, low light-dose lightsheet microscope LATTICE LIGHTSHEET
LATTICE LIGHTSHEET High-resolution, low light-dose lightsheet microscope First developed by Nobel Laureate Dr. Eric Betzig, the 3i Lattice LightSheet microscope is capable of imaging biological systems
More informationPrecision-tracking of individual particles By Fluorescence Photo activation Localization Microscopy(FPALM) Presented by Aung K.
Precision-tracking of individual particles By Fluorescence Photo activation Localization Microscopy(FPALM) Presented by Aung K. Soe This FPALM research was done by Assistant Professor Sam Hess, physics
More informationMulticolor 4D Fluorescence Microscopy using Ultrathin Bessel Light sheets
SUPPLEMENTARY MATERIAL Multicolor 4D Fluorescence Microscopy using Ultrathin Bessel Light sheets Teng Zhao, Sze Cheung Lau, Ying Wang, Yumian Su, Hao Wang, Aifang Cheng, Karl Herrup, Nancy Y. Ip, Shengwang
More informationBoulevard du Temple Daguerrotype (Paris,1838) a busy street? Nyquist sampling for movement
Boulevard du Temple Daguerrotype (Paris,1838) a busy street? Nyquist sampling for movement CONFOCAL MICROSCOPY BioVis Uppsala, 2017 Jeremy Adler Matyas Molnar Dirk Pacholsky Widefield & Confocal Microscopy
More informationDynamic Phase-Shifting Microscopy Tracks Living Cells
from photonics.com: 04/01/2012 http://www.photonics.com/article.aspx?aid=50654 Dynamic Phase-Shifting Microscopy Tracks Living Cells Dr. Katherine Creath, Goldie Goldstein and Mike Zecchino, 4D Technology
More informationExperimental protocol PIPE
Experimental protocol PIPE May 5, 2016 Abstract PIPE is a uorescence perturbation technique that works by measuring the expansion of a laser induced perturbation of photo convertible fused protein in the
More informationShreyash Tandon M.S. III Year
Shreyash Tandon M.S. III Year 20091015 Confocal microscopy is a powerful tool for generating high-resolution images and 3-D reconstructions of a specimen by using point illumination and a spatial pinhole
More informationMicroscope anatomy, image formation and resolution
Microscope anatomy, image formation and resolution Ian Dobbie Buy this book for your lab: D.B. Murphy, "Fundamentals of light microscopy and electronic imaging", ISBN 0-471-25391-X Visit these websites:
More informationLSM 710 Confocal Microscope Standard Operation Protocol
LSM 710 Confocal Microscope Standard Operation Protocol Basic Operation Turning on the system 1. Switch on Main power switch 2. Switch on System / PC power button 3. Switch on Components power button 4.
More informationConfocal Imaging Through Scattering Media with a Volume Holographic Filter
Confocal Imaging Through Scattering Media with a Volume Holographic Filter Michal Balberg +, George Barbastathis*, Sergio Fantini % and David J. Brady University of Illinois at Urbana-Champaign, Urbana,
More informationZeiss 780 Training Notes
Zeiss 780 Training Notes Turn on Main Switch, System PC and Components Switches 780 Start up sequence Do you need the argon laser (458, 488, 514 nm lines)? Yes Turn on the laser s main power switch and
More informationEUV microscopy - a user s perspective Dimitri Scholz EUV,
EUV microscopy - a user s perspective Dimitri Scholz EUV, 09.11.2011 Imaging technologies: available at UCD now and in the next future Begin ab ovo - Simple approaches direct to the goal - Standard methods
More informationLSM 780 Confocal Microscope Standard Operation Protocol
LSM 780 Confocal Microscope Standard Operation Protocol Basic Operation Turning on the system 1. Sign on log sheet according to Actual start time 2. Check Compressed Air supply for the air table 3. Switch
More informationPractical work no. 3: Confocal Live Cell Microscopy
Practical work no. 3: Confocal Live Cell Microscopy Course Instructor: Mikko Liljeström (MIU) 1 Background Confocal microscopy: The main idea behind confocality is that it suppresses the signal outside
More informationTRAINING MANUAL. Multiphoton Microscopy LSM 510 META-NLO
TRAINING MANUAL Multiphoton Microscopy LSM 510 META-NLO September 2010 Multiphoton Microscopy Training Manual Multiphoton microscopy is only available on the LSM 510 META-NLO system. This system is equipped
More informationNature Methods: doi: /nmeth Supplementary Figure 1
. Supplementary Figure 1 Schematics and characterization of our AO two-photon fluorescence microscope. (a) Essential components of our AO two-photon fluorescence microscope: Ti:Sapphire laser; optional
More informationMicroscopy Live Animal Imaging
Microscopy Live Animal Imaging A collaborative environment that provides the knowledge, instruments, and expertise needed to visualize life at scales ranging from single molecules to entire animals. Project
More informationSpectral Imaging with the Opterra Multipoint Scanning Confocal
Spectral Imaging with the Opterra Multipoint Scanning Confocal Outline Opterra design overview Scan Modes Light Path Spectral Imaging with Opterra Drosophila larva heart. Opterra Design Overview Supravideo
More informationOpterra. Multipoint Scanning Confocal Microscope. Innovation with Integrity. Cell-Friendly, High-Speed, High-Resolution Imaging
Opterra Multipoint Scanning Confocal Microscope Cell-Friendly, High-Speed, High-Resolution Imaging Innovation with Integrity Fluorescence Microscopy Opterra Multipoint Scanning Confocal Microscope Superior
More informationHoloMonitor M4. For powerful discoveries in your incubator
HoloMonitor M4 For powerful discoveries in your incubator HoloMonitor offers unique imaging capabilities that greatly enhance our understanding of cell behavior, previously unachievable by other technologies
More informationSUPPLEMENTARY INFORMATION
SUPPLEMENTARY INFORMATION Figure S1 Examples of spindles assembled on small chromatin bead structures. (a) Spindle assembled on a short string of aligned chromatinbeads. (b-d) Spindles assembled on chromatin-bead
More informationMegapixel FLIM with bh TCSPC Modules
Megapixel FLIM with bh TCSPC Modules The New SPCM 64-bit Software Abstract: Becker & Hickl have recently introduced version 9.60 of their SPCM TCSPC data acquisition software. SPCM version 9.60 not only
More informationLecture 16. OMX - Structured Illumination Microscopy Ian Dobbie x Microscopy Course Lecture 16 1
Lecture 16 OMX - Structured Illumination Microscopy Ian Dobbie x13323 Microscopy Course 2014 - Lecture 16 1 Super-resolution fluorescence microscopy Specificity Sensitivity Non-invasive (in situ & in vivo)
More informationPixel shift in fluorescence microscopy
Pixel shift in fluorescence microscopy 1. Introduction Multicolor imaging in fluorescence microscopy is typically performed by sequentially acquiring images of different colors. An overlay of these images
More informationattocfm I for Surface Quality Inspection NANOSCOPY APPLICATION NOTE M01 RELATED PRODUCTS G
APPLICATION NOTE M01 attocfm I for Surface Quality Inspection Confocal microscopes work by scanning a tiny light spot on a sample and by measuring the scattered light in the illuminated volume. First,
More informationFLUORESCENCE MICROSCOPY. Matyas Molnar and Dirk Pacholsky
FLUORESCENCE MICROSCOPY Matyas Molnar and Dirk Pacholsky 1 The human eye perceives app. 400-700 nm; best at around 500 nm (green) Has a general resolution down to150-300 μm (human hair: 40-250 μm) We need
More informationBi/BE 227 Winter Assignment #3. Adding the third dimension: 3D Confocal Imaging
Bi/BE 227 Winter 2016 Assignment #3 Adding the third dimension: 3D Confocal Imaging Schedule: Jan 20: Assignment Jan 20-Feb 8: Work on assignment Feb 10: Student PowerPoint presentations. Goals for this
More informationTissue Preparation ORGANISM IMAGE TISSUE PREPARATION. 1) Fixation: halts cell metabolism, preserves cell/tissue structure
Lab starts this week! ANNOUNCEMENTS - Tuesday or Wednesday 1:25 ISB 264 - Read Lab 1: Microscopy and Imaging (see Web Page) - Getting started on Lab Group project - Organ for investigation - Lab project
More informationHoriba Jobin-Yvon LabRam Raman Confocal Microscope (GERB 120)
Horiba Jobin-Yvon LabRam Raman Confocal Microscope (GERB 120) Please contact Dr. Amanda Henkes for training requests and assistance: 979-862-5959, amandahenkes@tamu.edu Hardware LN 2 FTIR FTIR camera 1
More informationSTORM/ PALM ANSWER KEY
STORM/ PALM ANSWER KEY Phys598BP Spring 2016 University of Illinois at Urbana-Champaign Questions for Lab Report 1. How do you define a resolution in STORM imaging? If you are given a STORM setup, how
More informationOpterra II Multipoint Scanning Confocal Microscope. Innovation with Integrity
Opterra II Multipoint Scanning Confocal Microscope Enabling 4D Live-Cell Fluorescence Imaging through Speed, Sensitivity, Viability and Simplicity Innovation with Integrity Fluorescence Microscopy The
More informationFast, high-contrast imaging of animal development with scanned light sheet based structured-illumination microscopy
nature methods Fast, high-contrast imaging of animal development with scanned light sheet based structured-illumination microscopy Philipp J Keller, Annette D Schmidt, Anthony Santella, Khaled Khairy,
More informationADVANCED METHODS FOR CONFOCAL MICROSCOPY II. Jean-Yves Chatton Sept. 2006
ADVANCED METHODS FOR CONFOCAL MICROSCOPY II Jean-Yves Chatton Sept. 2006 Workshop outline Confocal microscopy of living cells and tissues X-Z scanning Time series Bleach: FRAP, photoactivation Emission
More informationLab Report 3: Speckle Interferometry LIN PEI-YING, BAIG JOVERIA
Lab Report 3: Speckle Interferometry LIN PEI-YING, BAIG JOVERIA Abstract: Speckle interferometry (SI) has become a complete technique over the past couple of years and is widely used in many branches of
More informationNature Methods: doi: /nmeth Supplementary Figure 1. Schematic of 2P-ISIM AO optical setup.
Supplementary Figure 1 Schematic of 2P-ISIM AO optical setup. Excitation from a femtosecond laser is passed through intensity control and shuttering optics (1/2 λ wave plate, polarizing beam splitting
More informationFRAUNHOFER AND FRESNEL DIFFRACTION IN ONE DIMENSION
FRAUNHOFER AND FRESNEL DIFFRACTION IN ONE DIMENSION Revised November 15, 2017 INTRODUCTION The simplest and most commonly described examples of diffraction and interference from two-dimensional apertures
More informationImaging Retreat - UMASS Customized real-time confocal and 2-photon imaging
Imaging Retreat - UMASS 2012 Customized real-time confocal and 2-photon imaging Mike Sanderson Department of Microbiology and Physiological Systems University of Massachusetts Medical School Thanks for
More informationChapter 3 Broadside Twin Elements 3.1 Introduction
Chapter 3 Broadside Twin Elements 3. Introduction The focus of this chapter is on the use of planar, electrically thick grounded substrates for printed antennas. A serious problem with these substrates
More informationExperiment 1: Fraunhofer Diffraction of Light by a Single Slit
Experiment 1: Fraunhofer Diffraction of Light by a Single Slit Purpose 1. To understand the theory of Fraunhofer diffraction of light at a single slit and at a circular aperture; 2. To learn how to measure
More informationScanArray Overview. Principle of Operation. Instrument Components
ScanArray Overview The GSI Lumonics ScanArrayÒ Microarray Analysis System is a scanning laser confocal fluorescence microscope that is used to determine the fluorescence intensity of a two-dimensional
More informationOptical Sectioning Deep Inside Live Embryos by Selective Plane Illumination Microscopy
Supporting Online Material Optical Sectioning Deep Inside Live Embryos by Selective Plane Illumination Microscopy 1 Material and methods 1.1 Setup Jan Huisken, Jim Swoger, Filippo Del Bene, Joachim Wittbrodt,
More informationDepartment of Electrical Engineering and Computer Science
MASSACHUSETTS INSTITUTE of TECHNOLOGY Department of Electrical Engineering and Computer Science 6.161/6637 Practice Quiz 2 Issued X:XXpm 4/XX/2004 Spring Term, 2004 Due X:XX+1:30pm 4/XX/2004 Please utilize
More informationHigh resolution extended depth of field microscopy using wavefront coding
High resolution extended depth of field microscopy using wavefront coding Matthew R. Arnison *, Peter Török #, Colin J. R. Sheppard *, W. T. Cathey +, Edward R. Dowski, Jr. +, Carol J. Cogswell *+ * Physical
More informationNature Structural & Molecular Biology: doi: /nsmb Supplementary Figure 1
Supplementary Figure 1 Supplemental correlative nanomanipulation-fluorescence traces probing nascent RNA and fluorescent Mfd during TCR initiation. Supplemental correlative nanomanipulation-fluorescence
More informationOpti 415/515. Introduction to Optical Systems. Copyright 2009, William P. Kuhn
Opti 415/515 Introduction to Optical Systems 1 Optical Systems Manipulate light to form an image on a detector. Point source microscope Hubble telescope (NASA) 2 Fundamental System Requirements Application
More informationRapid Non linear Image Scanning Microscopy, Supplementary Notes
Rapid Non linear Image Scanning Microscopy, Supplementary Notes Calculation of theoretical PSFs We calculated the electrical field distribution using the wave optical theory developed by Wolf 1, and Richards
More informationThe DCS-120 Confocal Scanning FLIM System
he DCS-120 Confocal Scanning FLIM System he bh DCS-120 confocal scanning FLIM system converts a conventional microscope into a high-performance fluorescence lifetime imaging system. he system is based
More informationEvaluation of Confocal Microscopy. for Measurement of the Roughness of Deuterium Ice. Ryan Menezes. Webster Schroeder High School.
Evaluation of Confocal Microscopy for Measurement of the Roughness of Deuterium Ice Webster Schroeder High School Webster, NY Advisor: Dr. David Harding Senior Scientist Laboratory for Laser Energetics
More informationLeica TCS SP8 Quick Start Guide
Leica TCS SP8 Quick Start Guide Leica TCS SP8 System Overview Start-Up Procedure 1. Turn on the CTR Control Box, EL6000 fluorescent light source for the microscope stand. 2. Turn on the Scanner Power
More informationSupplementary Figure 2. Schematic of the outer ring and glass base incorporated with glass microfluidics.
Supplementary Figure 1. Image of compressor mount ~CM! and bottom side of coverslip compressor ~CC!. a: The CC will thread into the CM and will push down on a 25 mm coverslip that is nestled within the
More informationSUPPLEMENTARY INFORMATION
Optically reconfigurable metasurfaces and photonic devices based on phase change materials S1: Schematic diagram of the experimental setup. A Ti-Sapphire femtosecond laser (Coherent Chameleon Vision S)
More informationConfocal Laser Scanning Microscopy
Name of the Core Facility: Confocal Laser Scanning Microscopy CORE Forschungszentrum Immunologie Mainz Welcome to the CSLM Core Facility: The CLSM Core Facility enables working groups to incorporate high
More informationD2.1 Operating 2D STED Microscope
D2.1 Operating 2D STED Microscope Nature: Report Dissemination Level: Public Lead Beneficiary: UNIVDUN Author(s): Piotr Zdankowski Work Package: WP2 Task: ESR5 Version: 0.02 Last modified: 24/04/2017 Status:
More informationGuide to Confocal 5. Starting session
Guide to Confocal 5 Remember that when booking and before starting session you can check for any problems at https://www.bris.ac.uk/biochemistry/uobonly/cif/index.html Starting session Switch on microscope
More informationP202/219 Laboratory IUPUI Physics Department THIN LENSES
THIN LENSES OBJECTIVE To verify the thin lens equation, m = h i /h o = d i /d o. d o d i f, and the magnification equations THEORY In the above equations, d o is the distance between the object and the
More informationObservation of the Inner Structures of Sea-Urchin Eggs by Projection X-Ray Microscopy
Observation of the Inner Structures of Sea-Urchin Eggs by Projection X-Ray Microscopy K. Yada 1, K. Shinohara 2, Y. Hamaguchi 3 1 Aomori Public College, Aomori 030-01, Japan 2 Faculty of Medicine, The
More informationBio 407. Applied microscopy. Introduction into light microscopy. José María Mateos. Center for Microscopy and Image Analysis
Center for Microscopy and Image Analysis Bio 407 Applied Introduction into light José María Mateos Fundamentals of light Compound microscope Microscope composed of an objective and an additional lens (eyepiece,
More informationX-ray generation by femtosecond laser pulses and its application to soft X-ray imaging microscope
X-ray generation by femtosecond laser pulses and its application to soft X-ray imaging microscope Kenichi Ikeda 1, Hideyuki Kotaki 1 ' 2 and Kazuhisa Nakajima 1 ' 2 ' 3 1 Graduate University for Advanced
More informationUser Manual for HoloStudio M4 2.5 with HoloMonitor M4. Phase Holographic Imaging
User Manual for HoloStudio M4 2.5 with HoloMonitor M4 Phase Holographic Imaging 1 2 HoloStudio M4 2.5 Software instruction manual 2013 Phase Holographic Imaging AB 3 Contact us: Phase Holographic Imaging
More informationComparing FCS and FRAP as methodologies for calculating diffusion
Bi/BE 227 Winter 2018 Assignment #4 Comparing FCS and FRAP as methodologies for calculating diffusion Schedule: Jan 29: Assignment Jan 29-Feb 14: Work on assignment Feb 14: Student PowerPoint presentations.
More informationTCSPC at Wavelengths from 900 nm to 1700 nm
TCSPC at Wavelengths from 900 nm to 1700 nm We describe picosecond time-resolved optical signal recording in the spectral range from 900 nm to 1700 nm. The system consists of an id Quantique id220 InGaAs
More informationYou won t be able to measure the incident power precisely. The readout of the power would be lower than the real incident power.
1. a) Given the transfer function of a detector (below), label and describe these terms: i. dynamic range ii. linear dynamic range iii. sensitivity iv. responsivity b) Imagine you are using an optical
More informationTravel to New Dimensions- LSM 880. The Resolution of a Microscope is limited. The Resolution of a Microscope is limited. Image. Image. Object.
Travel to New Dimensions- LSM 880 LSM 880: The Power of Sensitivity Our Latest Member of the LSM 880 with GaAsP Detectors Sensitivity, and Ease of Use Innovative High-End Laser Scanning Microscopes from
More informationConfocal Raman Microscopy (WITec Alpha 300R)
Confocal Raman Microscopy (WITec Alpha 300R) Please refer to Witec Alpha300R Confocal Raman Microscope User Manual for the details of the operating procedure. Sample preparation 1. Attach your sample on
More informationLeica SP8 TCS Users Manual
Leica SP8 TCS Users Manual Follow the procedure for start up and log on as posted in the lab. Please log on with your account only and do not share your password with anyone. We track and confirm usage
More informationOperating Instructions for Zeiss LSM 510
Operating Instructions for Zeiss LSM 510 Location: GNL 6.312q (BSL3) Questions? Contact: Maxim Ivannikov, maivanni@utmb.edu 1 Attend A Complementary Training Before Using The Microscope All future users
More informationSensors and Metrology - 2 Optical Microscopy and Overlay Measurements
Sensors and Metrology - 2 Optical Microscopy and Overlay Measurements 1 Optical Metrology Optical Microscopy What is its place in IC production? What are the limitations and the hopes? The issue of Alignment
More informationNIH Public Access Author Manuscript Methods Cell Biol. Author manuscript; available in PMC 2014 July 15.
NIH Public Access Author Manuscript Published in final edited form as: Methods Cell Biol. 1998 ; 56: 185 215. A High-Resolution Multimode Digital Microscope System E. D. Salmon, Sidney L. Shaw, Jennifer
More informationFigure S1 Figure S1. Wild type IgG and FcRn colocalize in APPL+ TCs.
Figure S1 Figure S1. Wild type IgG and FcRn colocalize in APPL+ TCs. HMEC-1 cells were cotransfected with GFP-FcRn and β2m. Transfected cells were incubated with 200 μg/ml Alexa 647-wild type IgG (A) or
More informationsensicam em electron multiplication digital 12bit CCD camera system
sensicam em electron multiplication digital 12bit CCD camera system electron multiplication gain of up to 1000 superior resolution (1004 1002 pixel) for EMCCD extremely low noise < 1e excellent quantum
More informationOptical Microscopy and Imaging ( Part 2 )
1 Optical Microscopy and Imaging ( Part 2 ) Chapter 7.1 : Semiconductor Science by Tudor E. Jenkins Saroj Kumar Patra, Department of Electronics and Telecommunication, Norwegian University of Science and
More informationFigure 1. Oil-immersion objectives available for use with the Lionheart FX.
Tech Note Oil Objective Introduction The Lionheart FX automated imager is compatible with high numerical aperture oil immersion objectives. These objectives offer magnification up to 100X and significantly
More informationMOM#3: LIGHT SHEET MICROSCOPY (LSM) Stanley Cohen, MD
MOM#3: LIGHT SHEET MICROSCOPY (LSM) Stanley Cohen, MD Introduction. Although the technical details of light sheet imaging and its various permutations appear at first glance to be complex and require some
More informationLeica TCS SP8 Quick Start Guide
Leica TCS SP8 Quick Start Guide Leica TCS SP8 System Overview Start-Up Procedure 1. Turn on the CTR Control Box, Fluorescent Light for the microscope stand. 2. Turn on the Scanner Power (1) on the front
More informationEffects of spherical aberrations on micro welding of glass using ultra short laser pulses
Available online at www.sciencedirect.com Physics Procedia 39 (2012 ) 563 568 LANE 2012 Effects of spherical aberrations on micro welding of glass using ultra short laser pulses Kristian Cvecek a,b,, Isamu
More informationObserving Microorganisms through a Microscope LIGHT MICROSCOPY: This type of microscope uses visible light to observe specimens. Compound Light Micros
PHARMACEUTICAL MICROBIOLOGY JIGAR SHAH INSTITUTE OF PHARMACY NIRMA UNIVERSITY Observing Microorganisms through a Microscope LIGHT MICROSCOPY: This type of microscope uses visible light to observe specimens.
More information