Coherence-controlled holographic microscopy for live-cell QPI



Similar documents
Neuro imaging: looking with lasers in the brain

Holographically corrected microscope with a large working distance (as appears in Applied Optics, Vol. 37, No. 10, , 1 April 1998)

Optical Microscopy Quantifies Live Cells Without Labels

Z-Stacking and Z-Projection using a Scaffold-based 3D Cell Culture Model

Confocal Microscopy and Atomic Force Microscopy (AFM) A very brief primer...

Advances in scmos Camera Technology Benefit Bio Research

Optical Metrology. Third Edition. Kjell J. Gasvik Spectra Vision AS, Trondheim, Norway JOHN WILEY & SONS, LTD

Lecture 20: Scanning Confocal Microscopy (SCM) Rationale for SCM. Principles and major components of SCM. Advantages and major applications of SCM.

Color holographic 3D display unit with aperture field division

Microscopy. MICROSCOPY Light Electron Tunnelling Atomic Force RESOLVE: => INCREASE CONTRAST BIODIVERSITY I BIOL1051 MAJOR FUNCTIONS OF MICROSCOPES

A pretty picture, or a measurement? Retinal Imaging

Applications of confocal fluorescence microscopy in biological sciences

Chapter 4. Microscopy, Staining, and Classification. Lecture prepared by Mindy Miller-Kittrell North Carolina State University

Standard Test Method for Classification of Film Systems for Industrial Radiography 1

Preface Light Microscopy X-ray Diffraction Methods

5. Scanning Near-Field Optical Microscopy 5.1. Resolution of conventional optical microscopy

U.S. HOUSE OF REPRESENTATIVES COMMITTEE ON SCIENCE, SPACE, AND TECHNOLOGY Testimony

13 th CZECH DAYS FOR EUROPEAN RESEARCH CZEDER 2015

MIRAX SCAN The new way of looking at pathology

Zeiss Axioimager M2 microscope for stereoscopic analysis.

Today. next two weeks

NyONE - Cell imaging in a bird s eye view 4. NyONE...resolution matters! 8. Features & benefits 10. Fluorescence excitation channels 12

Fundamentals of modern UV-visible spectroscopy. Presentation Materials

RAY TRACING UNIFIED FIELD TRACING

A Brief History of the Microscope and its Significance in the Advancement of Biology and Medicine

ZEISS Microscopy Course Catalog

14 The ability of the lenses to distinguish fine detail and structure is called a. Illumination b. Magnification c. Refractive index d.

Practical Cell Analysis

Principles of Microscopy and Confocal and Fluorescence Microscopy

MICROSCOPY. To demonstrate skill in the proper utilization of a light microscope.

Web portal for information on cancer epidemiology in the Czech Republic

Near-field scanning optical microscopy (SNOM)

LASER APPLICATIONS IN MEDICINE AND BIOLOGY

Parameter inference of a basic p53 model using ABC

Fig.1. The DAWN spacecraft

Collagen I Self-Assembly: Revealing the Developing Structures that Generate Turbidity. Supporting Material

product overview pco.edge family the most versatile scmos camera portfolio on the market pioneer in scmos image sensor technology

Chapter 1 Parts C. Robert Bagnell, Jr., Ph.D., 2012

EXPERIMENT #1: MICROSCOPY

Diffraction of a Circular Aperture

Spherical Beam Volume Holograms Recorded in Reflection Geometry for Diffuse Source Spectroscopy

A down-under undergraduate optics and photonics laboratory

It has long been a goal to achieve higher spatial resolution in optical imaging and

Towards large dynamic range beam diagnostics and beam dynamics studies. Pavel Evtushenko

AFM-kit. Development of a kit for building from scratch an educational (but decently performing - i.e. usable) AFM.

VISUAL INSPECTION SYSTEMS

Servicio de Salud de Castilla-La Mancha

Scanning Near-Field Optical Microscopy for Measuring Materials Properties at the Nanoscale

Zeiss 780 Training Notes

These particles have something in common

PHYS 39a Lab 3: Microscope Optics

Spectroscopy Using the Tracker Video Analysis Program

Inspection and Illumination Systems for Visual Quality Assurance. Large selection Attractive prices Tailored solutions. optometron.

Fast Z-stacking 3D Microscopy Extended Depth of Field Autofocus Z Depth Measurement 3D Surface Analysis

Acousto-optic modulator

Project 2B Building a Solar Cell (2): Solar Cell Performance

Introduction to Flow Cytometry

This page intentionally left blank

Presentation and analysis of multidimensional data sets

Bio 321 Lightmicroscopy Electronmicrosopy Image Processing

Annexin V-EGFP Apoptosis Detection Kit

Basics of Image and data analysis in 3D

Czech Society for Experimental and Clinical Pharmacology and Toxicology, Czech Medical Association J. Ev.Purkyne Slovak Toxicology Society (SETOX)

FIFTH GRADE TECHNOLOGY

From apertureless near-field optical microscopy to infrared near-field night vision

use. 3,5 Apoptosis Viability Titration Assays

Biomedical Optics Theory

Chapter 13 Confocal Laser Scanning Microscopy C. Robert Bagnell, Jr., Ph.D., 2012

Status of the Free Electron Laser

MITOSIS IN ONION ROOT TIP CELLS: AN INTRODUCTION TO LIGHT MICROSCOPY

High speed 3D capture for Configuration Management DOE SBIR Phase II Paul Banks

Related topics: Application Note 27 Data Analysis of Tube Formation Assays.

Thermo Scientific ArrayScan XTI High Content Analysis Reader. revolutionizing cell biology with the power of high content

Opaque lenses. Allard Mosk Complex Photonic Systems MESA+, Universiteit Twente, The Netherlands

DOE Solar Energy Technologies Program Peer Review. Denver, Colorado April 17-19, 2007

Name: Due: September 21 st Physics 7230 Laboratory 3: High Resolution SEM Imaging

Introduction APPLICATION NOTE

ProScan DC Linear Servo Stage Technology

Application Note No. 2 / July Quantitative Assessment of Cell Quality, Viability and Proliferation. System

Chapter 12 Filters for FISH Imaging

Digital Holography using a Laser Pointer and Consumer Digital Camera Report date: June 22 nd, 2004

VECTORIAL ELECTRIC FIELD MONTE CARO SIMULA- TIONS FOR FOCUSED LASER BEAMS (800 nm 2220 nm) IN A BIOLOGICAL SAMPLE

Microscopy: Principles and Advances

Imaging and Bioinformatics Software

PHYSICAL METHODS, INSTRUMENTS AND MEASUREMENTS Vol. IV Femtosecond Measurements Combined With Near-Field Optical Microscopy - Artyom A.


Report of the Spectral Irradiance Comparison EURAMET.PR-K1.a.1 between MIKES (Finland) and NIMT (Thailand)

Optical laser beam scanner lens relay system

NEAR FIELD OPTICAL MICROSCOPY AND SPECTROSCOPY WITH STM AND AFM PROBES

Faculty of Electrical Engineering and Communication Brno University of Technology.

Scanning Near Field Optical Microscopy: Principle, Instrumentation and Applications

Application Note #503 Comparing 3D Optical Microscopy Techniques for Metrology Applications

Flow cytometry basics fluidics, optics, electronics...

Recording the Instrument Response Function of a Multiphoton FLIM System

Imaging with Second-HarmonicGeneration Nanoparticles. Chia-LungHsieh, Rachel Grange, Ye Pu, Demetri Psaltis \

Imaging techniques with refractive beam shaping optics

Image Analysis Using the Aperio ScanScope

Measuring the Point Spread Function of a Fluorescence Microscope

ISOLATION AND PROPERTIES OF SECRETORY GRANULES FROM RAT ISLETS OF LANGERHANS. II. Ultrastructure of the Beta Granule

AxioCam HR The Camera that Challenges your Microscope

Transcription:

SPIE Photonics West February 2015 Coherence-controlled holographic microscopy for live-cell QPI Tomáš Slabý, Aneta Křížová, Martin Lošťák, Jana Čolláková, Pavel Kolman, Zbyněk Dostál, Lukáš Kvasnica, Martin Antoš, Pavel Veselý, Radim Chmelík Institute of Physical Engineering, Faculty of Mechanical Engineering, Brno University of Technology Central European Institute of Technology, Brno University of Technology TESCAN Brno, s.r.o.

Coherence-controlled holographic microscopy (CCHM) CCHM is a technique for quantitative phase imaging (QPI) label-free no staining low light power densities low phototoxicity simple image segmentation quantitative cell dry-mass density measurements 1,2 based on off-axis holographic configuration single-shot technique fast acquisition (no scanning) adapted for incoherent illumination (halogen lamp) strong suppression of coherent noise (speckles) & parasitic interferences lateral resolution of convetional optical microscopes no image artifacts 1 R. Barer: Interference microscopy and mass determination. Nature 169, 1952, 366-367. 2 H. Davies, M. Wilkins: Interference microscopy and mass determination. Nature 169, 1952, 541.

Coherence-controlled holographic microscope (CCHM) based on off-axis holographic configuration adapted for incoherent illumination T. Slabý et al., Optics Express 21 (2013) 14747 CCHM prototype at Brno University of Technology

Coherence control Imaging properties of CCHM can be controlled by adjusting the degree of coherence spatial coherence is controlled by aperture diaphragm temporal coherence is controlled by bandpass filters Incoherent illumination strong suppression of coherence noise (speckles) & parasitic interferences improved lateral resolution up to factor of 2 coherence-gate effect Coherent illumination numerical refocusing in larger range

Coherence control elimination of speckles & parasitic interferences improved lateral resolution Resolution target, objective 10x/0.25 Incoherent halogen lamp + 650(10) nm filter Coherent HeNe laser (633 nm) T. Slabý et al., Optics Express 21 (2013) 14747

Coherence-gate effect specimen diffuser induced by incoherent illumination eliminates contribution of light scattered in out-offocus planes Observation of copper foil with rectangular holes covered with a diffuser T. Slabý et al., Optics Express 21 (2013) 14747 10x/0.25 650(10) nm filter brightfield CCHM amplitude CCHM phase

Increasing concentration of phospholipids Coherence-gated QPI in turbid medium Zernike PhC 0 % CCHM phase 0.15 % rat embryo fibroblasts K2 in flow chamber in emulsion of phospholipids with increasing concentration 0.3 % 1.5 % Zernike phase contrast is inapplicable at higher concentrations CCHM provides good contrast at higher concentrations and does not suffer from halo effect 20x/0.4 40x/0.65, 650(10) nm filter

Coherence-gated QPI in turbid medium human breast cancer cells MCF7 reaction to treatment by active phospholipid emulsion (0.5 %) observed in flow chamber 3 phase [rad] 20x/0.4, halogen lamp + 650(10) nm filter, total time 90 minutes 0

Coherence-gated QPI in turbid medium human breast cancer cells MCF7 reaction to treatment by active phospholipid emulsion (0.5 %) observed in flow chamber 3 phase [rad] 20x/0.4, halogen lamp + 650(10) nm filter, total time 90 minutes 0

Coherence-gated QPI in turbid medium colorectal cancer cells DLD1 reaction to treatment by active phospholipid emulsion (0.15 %) observed in flow chamber 20x/0.5, halogen lamp + 650(10) nm filter, total time 6 hours

Coherence-gated QPI in collagen gel human breast cancer cells MCF7 in collagen gel basic biological test of cancer cell invasivity recorded mechanism of cell motion, not detectable by common methods 20x/0.5, halogen lamp + 650(10) nm filter, total time 100 min

Dynamic phase differences method that makes slight changes more visible and enables dynamics evaluation and quantification mitosis of rat sarcoma cell K2 Phase t 0 Phase t 0 +τ Subtraction Area with increased mass New area with increased mass Area with decreased mass Abandoned area with decreased mass

Multimodal imaging human prostate cancer cells PC3 apoptosis detection combined holography and fluorescence imaging phase image (holography) Annexin V (fluorescence) 20x/0.5, halogen lamp + 650(10) nm filter In collaboration with RNDr. Jan Balvan, Faculty of Medicine, Masaryk University, Czech Republic

Multimodal imaging human prostate cancer cells PC3 combined holography and fluorescence imaging enables to clearly distinguish oncosis from apoptosis and to stratify the progression of oncosis In collaboration with RNDr. Jan Balvan, Faculty of Medicine, Masaryk University, Czech Republic

Conclusions Coherence-controlled holographic microscopy (CCHM) QPI with incoherent illumination Disadvantages more complicated set-up & alignment ( automated) Advantages speckle-free real-time QPI without image artifacts lateral resolution of convetional optical microscopes coherence-gate effect

Acknowledgements Experimental Biophotonics Group & Centre for Innovative Microscopy Radim Chmelík Zbyněk Dostál Martin Antoš Aneta Křížová Hana Uhlířová Veronika Jůzová Matěj Týč Michala Slabá Jiří Komrska Pavel Kolman Martin Lošťák Tomáš Zikmund Jana Čolláková Pavel Veselý Věra Kollarová Lukáš Kvasnica Petr Bouchal TESCAN Brno, s.r.o. Filip Lopour Josef Pokorný Václav Procházka Marek Minář This work was supported by Ministry of Industry and Trade of the Czech Republic (FR-TI4/660) CEITEC Central European Institute of Technology (CZ.1.05/1.1.00/02.0068) from European Regional Development Fund

Thank you for your attention