Jones Matrix Imaging for Transparent and Anisotropic Sample

Similar documents
Low Coherence Vibration Insensitive Fizeau Interferometer

Dynamic Complex Wavefront Modulation with an Analogue Spatial Light Modulator

ECEN 4606, UNDERGRADUATE OPTICS LAB

Metrology and Sensing

Two Dimensional SR-Interferometer at PETRA III. Artem Novokshonov DESY, Tomsk Polytechnic University

Figure measurement of a large optical flat with a Fizeau interferometer and stitching technique

Simple quasi-common path point diffraction interferometer with adjustable fringe contrast and carrier frequency

iprom Optical Interferometry Prof. Dr. -Ing. Rainer Tutsch Institut für Produktionsmesstechnik IPROM Technische Universität Braunschweig

Metrology and Sensing

Metrology and Sensing

One Type of Bio-Phase Microscopy Imaging Method Based on a Con Beam with Double Dove Prisms Jingrong Liao1, a, Jingye Liu2, b and Yuanyuan Xu2, c*

Experiment 5 Polarization and Modulation of Light

Using a Mach-Zehnder interferometer to measure the phase retardations of wave plates

PHY410 Optics Exam #3

Quantum information processing using linear optics

Fourier Transform Spectrograph Development Project

Comparative Measurement in Speckle Interferometry using Fourier Transform

Polarization of Light and Birefringence of Materials

Astronomy 203 practice final examination

Metrology and Sensing

Introduction to Interferometer and Coronagraph Imaging

Visualization of Convective Structures by Methods of the Hilbert Optics and Phase-Shift Interferometry

: Imaging Systems Laboratory II. Laboratory 6: The Polarization of Light April 16 & 18, 2002

16. More About Polarization

Identifying the crystal orientation of the black phosphorus

Effects of birefringence on Fizeau interferometry that uses polarization phase shifting technique

Supporting Information

Analysis of the signal fall-off in spectral domain optical coherence tomography systems

Lab 2: Single Photon Interference

Development of a cryogenic compact interferometric displacement sensor

Optics.

Supplementary Materials for

14. Matrix treatment of polarization

Edward S. Rogers Sr. Department of Electrical and Computer Engineering. ECE318S Fundamentals of Optics. Final Exam. April 16, 2007.

Birefringence dispersion in a quartz crystal retrieved from a channelled spectrum resolved by a fibre-optic spectrometer

Polarization Shearing Interferometer (PSI) Based Wavefront Sensor for Adaptive Optics Application. A.K.Saxena and J.P.Lancelot

2.71. Final examination. 3 hours (9am 12 noon) Total pages: 7 (seven) PLEASE DO NOT TURN OVER UNTIL EXAM STARTS PLEASE RETURN THIS BOOKLET

A Digital Holographic Approach for Co-Phasing of Segmented Telescopes: Proof of Concept Using Numerical Simulations

1. Consider the biconvex thick lens shown in the figure below, made from transparent material with index n and thickness L.

Phys 531 Lecture 27 6 December 2005

Use of computer generated holograms for alignment of complex null correctors

Thermal Imaging at Multiple Time Instants for Study of Self-Heating and ESD Phenomena

Polarization division multiplexing system quality in the presence of polarization effects

Optical Systems Program of Studies Version 1.0 April 2012

Real-time control of the periodicity of a standing wave: an optical accordion

Designing a Computer Generated Hologram for Testing an Aspheric Surface

LAB DEMONSTRATION OF INTERFEROMETRIC

17. Jones Matrices & Mueller Matrices

Parallel fractional correlation: implementation

Single-shot measurement of free-electron laser polarization at SDUV-FEL

QUANTUM- CLASSICAL ANALOGIES

Physics of Light and Optics

arxiv: v1 [quant-ph] 18 Mar 2008

Experimental generalized contextuality with single-photon qubits: supplementary material

Advanced techniques Local probes, SNOM

Scattering of Poincaré beams: polarization speckles

arxiv: v3 [physics.optics] 4 Feb 2016

COMPLEX OPTICAL FIELDS GENERATION USING A VECTORIAL OPTICAL FIELD GENERATOR

Interference. Reminder: Exam 2 and Review quiz, more details on the course website

Complex data mapping on a binary ferroelectric liquid crystal electrically addressed spatial light modulator for target recognition

Spectral Calibration of Ultra- High Resolution Volume Holographic Spectrometer. Jeff Bourne Majid Badiei (Advisor)

Phase-Shifting Interferometry and Combined Methods

DIGITAL CORRELATION OF FIRST ORDER SPACE TIME IN A FLUCTUATING MEDIUM

Laser Speckle and Applications in Optics

arxiv:quant-ph/ v1 30 Sep 2005

Quantum state measurement

First observations of the second solar spectrum with spatial resolution at the Lunette Jean Rösch

ANSYS-Based Birefringence Property Analysis of Side-Hole Fiber Induced by Pressure and Temperature

Optical Simulation Analysis of a Geometrical-phase-based. Nulling Interferometer

Physics 313: Laboratory 8 - Polarization of Light Electric Fields

Two-electron systems

COMPUTER GENERATED HOLOGRAMS Optical Sciences 627 W.J. Dallas (Monday, August 23, 2004, 12:14 PM)

Final examination. 3 hours (9am 12 noon) Total pages: 7 (seven) PLEASE DO NOT TURN OVER UNTIL EXAM STARTS PLEASE RETURN THIS BOOKLET

VELOCITY MEASUREMENTS IN CAPILLARIES

Path Entanglement. Liat Dovrat. Quantum Optics Seminar

Fourier Transform Infrared. Spectrometry

Chap. 5. Jones Calculus and Its Application to Birefringent Optical Systems

Sampling Theorem for Surface Profiling by White-Light Interferometry

Spectroscopic Measurements of Optical Elements For Submillimeter Receivers

Efficient sorting of orbital angular momentum states of light

Advanced Optical Coherence Tomography techniques: novel and fast imaging tools for non-destructive testing

-enlightening-the-future- Santiago de Compostela, August Session papers

High resolution tomographic diffraction microscopy

GRATING CLASSIFICATION

Recent progress in SR interferometer

OPTI510R: Photonics. Khanh Kieu College of Optical Sciences, University of Arizona Meinel building R.626

Characterization of Entanglement Photons Generated by a Spontaneous Parametric Down-Conversion Pulse Source

Fish embryo multimodal imaging by laser Doppler digital holography

Gratings in Electrooptic Polymer Devices

OPTI510R: Photonics. Khanh Kieu College of Optical Sciences, University of Arizona Meinel building R.626

The science of light. P. Ewart

Aerial image based lens metrology for wafer steppers

홀로그램저장재료. National Creative Research Center for Active Plasmonics Applications Systems

Particle-Wave Duality and Which-Way Information

Density Field Measurement by Digital Laser Speckle Photography

Electricity&Magnetism Lecture 24. Electricity & Magne/sm Lecture 24, Slide 1

Where are the Fringes? (in a real system) Div. of Amplitude - Wedged Plates. Fringe Localisation Double Slit. Fringe Localisation Grating

F 44 Normal Zeeman Effect

Determination of Young s modulus of glass by Cornu s apparatus

Physics I Keystone Institute Technology & Management Unit-II

Transcription:

ones Matrix Imaging for Transparent and Anisotropic Sample Theor of ones Matrix: The plane wave components of the optical field can be written as: )) ( exp( ), ( 0 x x x kz t i t z )) ( exp( ), ( 0 kz t i t z x i x x e 0 i e 0 x i o i x x e e 0 According to ones matrix formalism, x = xx x + x = x x + x x x xx x ' ' For example the linear polarizer is characterized b the relation: x x x P ' P ' x x x P P 0 0 ' ' 0 Px, 1 1

Applications of ones Matrix To understand the light matter interaction To measure the stress and strain in materials In biolog - for diagnosis of diseases In cosmetic industries To understand the propagation of light through several polarizing elements xperimental techniques to determine ones Matrix ones phase microscop (PM) of transparent and anisotropic sample Polarization Holographic Microscop (PHM) 2

ones phase microscop (PM) of transparent and anisotropic sample Basic Principle: The ones matrix of sample is described as: xx x x To retrieve complete ones matrix +45 and -45 linearl polarized input beam is given to sample. 1 1 45 C 1 45 C 2 1 1 Y Y 11 12 Y Y Y Y C 11 21 12 22 1 xx x x C1 C2 0 0 C C 0 0 1 2 0 0 C C Y Y 1 2 21 22 C 0 0 C 1 C 2 2 xx x x xx x x xperimental setup: Ref.- Zhuo Wang, Larr. Millet, Martha U. Gillette, and Gabriel Popescu, Opt.Lett.33, (2008), 1270 Figure - xperimental setup of ones Phase Microscop [3], P 0, P R and P A polarizer, C 1, C 2 collimating lenses, L1, L2 Fourier lens pair, BS beam splitter, CCD charge coupled device Requires Four Steps Not applicable for dnamic object 3

Polarization Holographic Microscop (PHM) for ones Matrix Imaging Figure - xperimental setup for Polarization Holographic Microscop Ref.-Youngchan Kim, oonwoo eong, aeduck ang, Mahn Won Kim, and YongKeun Park, Opt.xp.20, (2012), 9949. 4

Advantages: Our Proposed Technique Requires two steps In our proposed experimental technique, triangular Sagnac interferometer provides freedom to adjust carrier frequencies according to sampling law. Basic Principle: Y Y x = xx x + x ' x xx x x = x x + ' x For +45 input beam 11 12 xx x x 1 1 11 12 xobject xwo.. object object wo.. object 11 12 xx x x 5

Our Proposed Technique (Double Shot) Basic Principle: Similarl for +45 input beam xperimental Setup: Y Y 21 22 21 xx x xx x 1 1 x SF 22 xx x x 1 2 1 2 1 2 1 2 x 11 11 12 12 21 21 22 22 CCD - GX 2750 with specifications A/D 14-bit, 2750 2200 pixels and pixel pitch 4.54 μm. Figure - xperimental Setup of ones matrix imaging; BS - Beam splitter, PBS - polarization beam splitter, M1, M2, M3 mirrors, HWP - half wave plate, SF spatial filter, CCD charge couple device, L1, L2, L3, L4,L5 lenses Ref.: N. K. Soni, A. S. Somkuwar and R. K. Singh," ones matrix imaging for transparent and anisotropic sample", Proc. SPI9654, International Conference on Optics and Photonics 2015, 965420 (une 15, 2015); doi:10.1117/12.2181657; http://dx.doi.org/10.1117/12.2181657. 6

xperimental Results: 1) ones matrix for complete transmission 1 0 0 1 (a) (b) (c) (d) Figure - Interferogram recorded for (a) +45 linearl polarized beam without sample (b)+45 linearl polarized beam with sample (c) -45 linearl polarized beam without sample (d) )-45 linearl polarized beam with sample 7

Fourier Fringe Analsis Technique F.T. x Amplitude Phase I.F.T. Two orthogonal polarization components are simultaneousl retrieved through Fourier Fringe Analsis 8

1) ones matrix for complete transmission 1 0 0 1 (a) (b) (c) (d) (e) (f) (g) (h) Figure - ones matrix components for complete transmission ; (a), (c), (e), (g) amplitude distributions of xx, x, x, ; (b), (d), (f), (h) phase distributions of xx, x, x, ; 9

2) ones matrix for horizontal polarizer 1 0 0 0 (a) (b) Figure - xperimentall recorded hologram for (a) +45 (b)-45 illumination beam (a) (b) (c) (d) (e) (f) (g) (h) Figure - ones matrix components for horizontal polarizer ; (a), (c), (e), (g) amplitude distributions of xx, x, x, ; (b), (d), (f), (h) phase distributions of xx, x, x, ; 10

3) ones matrix for vertical polarizer 0 0 0 1 (a) (b) Figure - xperimentall recorded hologram for (a) +45 (b)-45 illumination beam (a) (b) (c) (d) (e) (f) (g) (h) Figure - ones matrix components for vertical polarizer ; (a), (c), (e), (g) amplitude distributions of xx, x, x, ; (b), (d), (f), (h) phase distributions of xx, x, x, ; 11

4) ones Matrix for quarter wave plate with fast axis aligned at horizontal 1 0 0 i (a) Figure - xperimentall recorded interferogram for (a) +45 (b)-45 illumination beam (b) (a) (b) (c) (d) (e) (f) (g) (h) Figure - ones matrix components for QWP with fast axis aligned at horizontal ; (a), (c), (e), (g) amplitude distributions of xx, x, x, ; (b), (d), (f), (h) phase distributions of xx, x, x, 12 ;

Single Shot ones Microscop Limitations Of double shot ones matrix imaging: xperimental Setup: M1 M2 Not applicable for dnamic objects Highl Sensitive for vibration and atmospheric air fluctuations Advantages of Single Shot ones Microscop: Requires onl one measurement Applicable for dnamic objects also Y 11 Y 21 Y 12 Y 22 M4 Capable to tune spatial frequencies Fourier spectrum M3 No need of special optical elements like grating Figure-Single Shot ones Microscop 13

xperimental Results 1.Vertical polarizer Interferogram Amplitude of Fourier spectrum 14

1.Vertical polarizer 0 0 0 1 (a) (b) (c) (d) (e) (f) (g) (h) Figure - ones matrix components for vertical polarizer ; (a), (c), (e), (g) amplitude distributions of xx, x, x, ; (b), (d), (f), (h) phase distributions of xx, x, x, ; 15

2.Horizontal Polarizer Interferogram Amplitude of Fourier spectrum 16

2.Horizontal Polarizer 1 0 0 0 (a) (b) (c) (d) (e) (f) (g) (h) Figure - ones matrix components for horizontal polarizer ; (a), (c), (e), (g) amplitude distributions of xx, x, x, ; (b), (d), (f), (h) phase distributions of xx, x, x, ; 17

3.Polarizer @45 Interferogram Amplitude of Fourier spectrum 18

3.Polarizer @45 0.5 0.5 0.5 0.5 (a) 396 μm 396 μm (b) 396 μm (c) 396 μm (d) (e) 396 μm 396 μm (f) 396 μm (g) 396 μm (h) Figure - ones matrix components for polarizer at 45; (a), (c), (e), (g) amplitude distributions of xx, x, x, ; (b), (d), (f), (h) phase distributions of xx, x, x, ; 19

4.Polarizer @-45 Interferogram Amplitude of Fourier spectrum 20

4.Polarizer @-45 0.5 0.5 0.5 0.5 (a) (b) (c) (d) (e) (f) (g) (h) Figure - ones matrix components for polarizer at -45; (a), (c), (e), (g) amplitude distributions of xx, x, x, ; (b), (d), (f), (h) phase distributions of xx, x, x, ; 21

5.Half wave plate @0 Interferogram Amplitude of Fourier spectrum 22

5.Half wave plate @0 1 0 0 1 (a) (b) (c) (d) (e) (f) (g) (h) Figure - ones matrix components for half wave plate at 0 degree; (a), (c), (e), (g) amplitude distributions of xx, x, x, ; (b), (d), (f), (h) phase distributions of xx, x, x, ; 23

6.Half wave plate @90 Interferogram Amplitude of Fourier spectrum 24

6.Half wave plate @90 1 0 0 1 (a) (b) (c) (d) (e) (f) (g) (h) Figure - ones matrix components for half wave plate at 90; (a), (c), (e), (g) amplitude distributions of xx, x, x, ; (b), (d), (f), (h) phase distributions of xx, x, x, ; 25

7.Half wave plate @45 Interferogram Amplitude of Fourier spectrum 26

7.Half wave plate @45 0 1 1 0 (a) (b) (c) (d) (e) (f) (g) (h) Figure - ones matrix components for half wave plate at 45; (a), (c), (e), (g) amplitude distributions of xx, x, x, ; (b), (d), (f), (h) phase distributions of xx, x, x, ; 27

8.QWP @0 Interferogram Amplitude of Fourier spectrum 28

8.QWP @0 1 0 0 i (a) (b) (c) (d) (e) (f) (g) (h) Figure - ones matrix components for vertical polarizer ; (a), (c), (e), (g) amplitude distributions of xx, x, x, ; (b), (d), (f), (h) phase distributions of xx, x, x, ; 29

9.QWP @90 Interferogram Amplitude of Fourier spectrum 30

9.QWP @90 1 0 0 i (a) (b) (c) (d) (e) (f) (g) (h) Figure - ones matrix components for quarter wave plate at 90; (a), (c), (e), (g) amplitude distributions of xx, x, x, ; (b), (d), (f), (h) phase distributions of xx, x, x, ; 31

10.PVA Interferogram Amplitude of Fourier spectrum 32

10. Polvinl Alcohol (PVA) (a) (b) (c) (d) (e) (f) (g) (h) Figure - ones matrix components for vertical polarizer ; (a), (c), (e), (g) amplitude distributions of xx, x, x, ; (b), (d), (f), (h) phase distributions of xx, x, x, ; 33

11.Human Hair Interferogram Amplitude of Fourier spectrum 34

11.Human Hair (a) (b) (c) (d) (e) (f) (g) (h) Figure - ones matrix components for human hair; (a), (c), (e), (g) amplitude distributions of xx, x, x, ; (b), (d), (f), (h) phase distributions of xx, x, x, ; 35

12.Blood Sample Interferogram Amplitude of Fourier spectrum 36

12. ones matrix components for Blood Sample 99 μm 99 μm 99 μm 99 μm 99 μm 99 μm 99 μm 99 μm Figure - ones matrix components for blood sample; (a), (c), (e), (g) amplitude distributions of xx, x, x, ; (b), (d), (f), (h) phase distributions of xx, x, x, ; 37