FIBER-OPTIC LASER INTERFEROMETER FOR VISION RESEARCH Timne Bilton PI & Supervisor: Dr. David Williams Collaborators: Julianna Lin, Silvestre Manzanera.

Slides:



Advertisements
Similar presentations
Introduction to Eye Tracking
Advertisements

Waveguide group velocity determination by spectral interference measurements in NSOM Bill Brocklesby Optoelectronics Research Centre University of Southampton,
Lab 1 Paraxial Optics Lab in 106A. Look at paraxial optics rules Use a bi-convex singlet at 1:1 conjugates Do it double pass so can see image Lateral.
LIGHT AND THE RETINAL IMAGE: KEY POINTS Light travels in (more or less) straight lines: the pinhole camera’s inverted image Enlarging the pinhole leads.
4/13/2017 5:04 PM Diffraction © 2007 Microsoft Corporation. All rights reserved. Microsoft, Windows, Windows Vista and other product names are or may be.
The Wave Nature of Light
Your vision and optical illusions - A story about the most important sense and the way we use it.
Topic 11.3 Diffraction.
Electromagnetic Waves G3 Two Source Interference of Waves G4 The Diffraction Grating.
Foundations of Physics
Unit 33 - Optics Optics is the study of the behavior and properties of light. This includes it’s interactions with objects including mirrors, lenses, and.
Adaptive Optics Deformable Mirror Electronics Simulation Pearl Yamaguchi Subaru Telescope National Astronomical Observatory of Japan Mentor: Stephen Colley.
1 Laser Beam Coherence Purpose: To determine the frequency separation between the axial modes of a He-Ne Laser All sources of light, including lasers,
Digital Image Processing: Digital Imaging Fundamentals.
Adaptive Optics and Optical Interferometry or How I Learned to Stop Worrying and Love the Atmosphere Brian Kern Observational Astronomy 10/25/00.
Optical Alignment with Computer Generated Holograms
Amplitude Control: Closing the Loop in a Zero Path Length Difference Michelson Interferometer Michael G. Littman, Michael Carr , Laurent Pueyo, Jeremy.
Phase and Amplitude Control Ability using Spatial Light Modulators and Zero Path Length Difference Michelson Interferometer Michael G. Littman, Michael.
Newton’s Rings Another method for observing interference in light waves is to place a planoconvex lens on top of a flat glass surface, as in Figure 24.8a.
Diffraction vs. Interference
Dr. Curtis Banks Mentor EV-43 Harvesting Environmental White Noise to Perform Structural Health Monitoring with Fiber Bragg Grating Sensors Justin Colar.
Lecture 14 Images Chapter 34 Geometrical Optics Fermats Principle -Law of reflection -Law of Refraction Plane Mirrors and Spherical Mirrors Spherical refracting.
Figure 2.1 Block diagram of a generic projection imaging system.
The wave nature of light Interference Diffraction Polarization
Visual Angle How large an object appears, and how much detail we can see on it, depends on the size of the image it makes on the retina. This, in turns,
Double-Dynamic Interferometry in IR and Visible in Semiconductor Crystals P. Land†, N. Kukhtarev*, T. Kukhtareva, and J. C. Wang Department of Physics,
ECE 299 Holography and Coherent Imaging Lecture 1 Gabor Holography David J. Brady Duke University Lecture 1: Gabor Holographywww.disp.duke.edu/~dbrady/courses/holography.
Vasilios Aris Morikis Dan DeLahunta Dr. Hyle Park, Ph.D.
IPBSM status and plan ATF project meeting M.Oroku.
LASER AND ADVANCES IN METROLOGY
“Twinkle, Twinkle Little Star”: An Introduction to Adaptive Optics Mt. Hamilton Visitor’s Night July 28, 2001.
Austin Roorda, Ph.D. University of Houston College of Optometry
1 Characterization of a Bimorph Deformable Mirror in a Closed Loop Adaptive Optics System for Vision Science Purposes Zachary Graham 1 Sophie Laut 2, David.
Characterization and Upgrading of Adaptive Optics Demonstrator Joseph Curamen Maui Community College Mark Hoffman & Mark Ammons MCC & UCSC-CfAO.
Modern Optics Lab Lab 6 Part 2: Interference Experiments  Observe interference by plane-parallel plates: Measure the thickness of the plates based on.
Optics Observations Pinholes, apertures and diffraction
Lenses Chapter 30. Converging and Diverging Lenses  Lens – a piece of glass which bends parallel rays so that they cross and form an image  Converging.
Transverse or longitudinal waves transport energy from one point to another. Each particle in the medium vibrates or oscillates, and disturbs the neighbouring.
Chapters 21 & 22 Interference and Wave Optics Waves that are coherent can add/cancel Patterns of strong and weak intensity.
Holography and temporal coherence Coherence lengths required?
Actuator 2 – Provides rotation about the roll direction. Actuator 1 – Provides rotation about the pitch direction Figure 2: The Linear Actuator model Abstract.
Electromagnetic Waves G3 Two Source Interference of Waves G4 The Diffraction Grating G5 X-Ray Diffraction.
DECREASED FLICKER SENSITIVITY WITH A SCANNED LASER DISPLAY. J.P. Kelly 1, H.L. Pryor, E.S. Viirre, T. Furness III. 1 Children's Hospital & Medical Center;
1.Stable radiation source 2.Wavelength selector 3.Transparent sample holder: cells/curvettes made of suitable material (Table 7- 2) 4.Radiation detector.
Improved Image Quality in AO-OCT through System Characterization
Why isn’t vision perfect? An exercise in psychoanatomy.
University of Kurdistan Digital Image Processing (DIP) Lecturer: Kaveh Mollazade, Ph.D. Department of Biosystems Engineering, Faculty of Agriculture,
I.Introduction II. System Design B.E. Unks, N. A. Proite, D. D. Yavuz University of Wisconsin – Madison The above figure shows a block diagram of the apparatus.
University of Latvia Trends in Physics, Budapest, Hungary Electro-optical solution for visual acuity and contrast sensitivity modeling Roberts Paeglis.
Virtual Retinal Display (VRD) Emulator Test System H.L. Pryor, B. Burstein, J. Kollin, E.S. Viirre, E. Seibel, J.P. Kelly, T. Furness III. Human Interface.
Adaptive Optics in the VLT and ELT era Optics for AO
For off-center points on screen, Fresnel zones on aperture are displaced …harder to “integrate” mentally. When white and black areas are equal, light at.
Optical Instruments II Instruments for Imaging the Retina.
Optical Sciences CenterThe University of Arizona ERROR ANALYSIS FOR CGH OPTICAL TESTING Yu-Chun Chang and James Burge Optical Science Center University.
Date of download: 6/25/2016 Copyright © 2016 SPIE. All rights reserved. Schematic optical layout of the instrument. Color box legend: Upright optical tweezers.
Date of download: 6/28/2016 The Association for Research in Vision and Ophthalmology Copyright © All rights reserved. From: A Novel, Real-Time, In.
University of Rochester, Center for Visual Science The Use of a MEMS Mirror for Adaptive Optics in the Human Eye Nathan Doble 1, Geun-Young Yoon 1, Li.
From: A Review of Adaptive Optics Optical Coherence Tomography: Technical Advances, Scientific Applications, and the Future Invest. Ophthalmol. Vis. Sci..
From: Focus information is used to interpret binocular images
From: Binocular visual acuity for the correction of spherical aberration in polychromatic and monochromatic light Journal of Vision. 2014;14(2):8. doi: /
Digital Image Processing (DIP)
3D Holographic Technology
Bill Brocklesby Optoelectronics Research Centre
From: A Novel, Real-Time, In Vivo Mouse Retinal Imaging System
Holography and temporal coherence
MICHELSON INTERFEROMETER
Review calculation of Fresnel zones
“Twinkle, Twinkle Little Star”: An Introduction to Adaptive Optics
Fig. 1 Experimental setup.
Temporal Error Minimization In Adaptive Optics Control Loop
Presentation transcript:

FIBER-OPTIC LASER INTERFEROMETER FOR VISION RESEARCH Timne Bilton PI & Supervisor: Dr. David Williams Collaborators: Julianna Lin, Silvestre Manzanera & Sapna Shroff University of Rochester Center for Visual Science & Dept of Electrical and Computer Engineering

OBJECTIVE To design and calibrate a fiber coupled laser interferometer to be used in conjunction with the University of Rochester’s adaptive optics ophthalmoscope. 1

Laser interferometry avoids blur from diffraction and aberrations WHAT IS INTERFEROMETRY APPLIED TO THE EYE? 2

WHY USEFUL IN VISION? Eye’s optical aberrations primarily limit vision and retinal imaging. Adaptive optics reduces these aberrations, but image quality is still diffraction- limited by the pupil. Laser interferometry can image fringes on that retina that are immune to blur from diffraction as well as aberrations 3

APPLICATIONS Measuring neural visual performance (CSF) Retinal image resolution exceeding the diffraction limit using structured illumination 4

STRUCTURED ILLUMINATION Simulation of imaging interference fringes onto the cone mosaic Retinal images taken with AO should contain moire patterns such as simulated below when the fringe frequency is 130 cycles/deg Such moire patterns may contain valuable information about the cone mosaic as well as other retinal structures Sampling Frequency

DESIGN 690 nm fiber coupled laser is connected to a fiber splitter The splitter feeds directly to two acousto-optic modulators The altered beams are reflected off a right angle prismatic mirror through a series of relay mirrors and a galvanometer Light is sent to the pupil plane via the AO system Fiber modulator Fiber-coupled laser Fiber splitter (1x2) Fiber modulator Lens Mirror on galvanometer Lens Focusing Lens Mirror Movable platform Right Angle Mirror 6

CONTRAST CONTROL WITH ACOUSTO-OPTIC MODULATORS AOMs will pulse the light beams delivered to the retina 500 times a second. Pulses arriving simultaneously generate fringe contrast is 100%. Phase delays bring contrast down towards zero Digital control of pulse overlap alters fringe contrast easily 7

BUILDING Clockwise from the left: Construction and alignment process. Bite bar for head stabilization Assembled (inset) prismatic mirror and U- bench holding fiber cable 8

ZEMAX SIMULATION An approximate fringe image was generated by generating a lens modeling system. Resolution of this image was limited to the ability of the computer’s memory EFL, FFD and BFD determined by designer calculations 9 TOP: Fringe Diagram at retinal plane LEFT: Unfolded Layout of system (after prismatic mirror)

SPATIAL FREQUENCY CALIBRATION Ronchi rulings (transparent plate ruled with black lines and clear spaces of equal width) of known frequency placed in a conjugate retinal plane Frequency match will be made by adjusting the fringe frequency until the Moiré pattern formed with the Ronchi ruling was zero spatial frequency. U bench position will be recorded when interference fringe has identical frequency. 10

RESULTS Low contrast fringes were observed  able to see magnified fringes on a piece of paper, but disappear later in the system Unexpected vibrations made fringe imaging inconsistent Laser issue: temporal coherence required for contrast  current of the laser was below the threshold current for lasing 11

ACKNOWLEDGEMENTS David R. Williams, PhD Center for Visual Science, University of Rochester Center for Adaptive Optics, University of California at Santa Cruz College of Optical Sciences, University of Arizona This project is supported by a Research Experiences for Undergraduates (REU) supplement to the National Science Foundation and Technology Center for Adaptive Optics, managed by the University of California at Santa Cruz under A cooperative agreement No. AST

REFERENCES Publications: Miller, D., Williams, D.R., Morris, G.M., and Liang, J. (1996) Images of cone photoreceptors in the living human eye. Vision Res., 36, DOI link: doi: / (95) DOI link Liang, J., Williams, D.R., and Miller, D.T. (1997) Supernormal vision and high resolution retinal imaging through adaptive optics. J. Opt. Soc. Am. A., 14, H. Hofer, L. Chen, G. Y. Yoon, B. Singer, Y. Yamauchi, and D. R. Williams, (2001) Improvement in retinal image quality with dynamic correction of the eye's aberrations. Optics Express 8, MacRae, S., Williams, D.R., (2001) Wavefront Guided Ablation. American Journal of Ophthalmology, 132:6, Wikipedia-The Free Encyclopedia ( 13