Data Collection and Analysis Theory Motivation A Study of Propagation of Laser Light through a Turbulent Atmosphere MIDN 3/C Meredith L. Lipp Professor.

Slides:



Advertisements
Similar presentations
The Wave Nature of Light
Advertisements

The Impact of Channel Estimation Errors on Space-Time Block Codes Presentation for Virginia Tech Symposium on Wireless Personal Communications M. C. Valenti.
Observation of the relativistic cross-phase modulation in a high intensity laser plasma interaction Shouyuan Chen, Matt Rever, Ping Zhang, Wolfgang Theobald,
1 Transmission Fundamentals Chapter 2 (Stallings Book)
Chapter-3-1CS331- Fakhry Khellah Term 081 Chapter 3 Data and Signals.
Communication as an Engineering Problem 1. Communication requirement #1 1)There must be some characteristic of the receiver’s environment that can be.
Svetlana Avramov-Zamurovic, Reza Malek-Madani, U.S. Naval Academy Olga Korotkova, University of Miami.
Analysis of Laser Light Propagation Midshipman 1/C Daniel Joseph Whitsett MIDN 4/C Joe Dinkel MIDN 4/C Meredith Lipp Professor Svetlana Avramov-Zamurovic.
TRANSMISSION FUNDAMENTALS Review
Probability density function of partially coherent beams propagating in the atmospheric turbulence Olga Korotkova, Physics Department, University of Miami,
April 2003 Mohit Garg, IIT Bombay 1 Free Space Optical Communication Picture:
ECE 4321 Computer Networks Chapter 4 Transmission Media: Wireless.
Jayasri Akella Error Analysis of Multi-Hop Free-Space Optical Communication Jayasri Akella, Murat Yuksel, Shiv Kalyanaraman Department of Electrical, Computer.
1 Mobile Communication Systems 1 Prof. Carlo Regazzoni Prof. Fabio Lavagetto.
Modeling OFDM Radio Channel Sachin Adlakha EE206A Spring 2001.
Digital Image Processing Chapter 5: Image Restoration.
Lecture 3 – Physical Optics
(1) Feature-point matching by D.J.Duff for CompVis Online: Feature Point Matching Detection, Extraction.
VTSLM images taken again at (a) 4.5  (T=84.7K), (b) 3.85  (T=85.3K), (c) 22.3  (T=85.9K), and (d) 31.6  (T=86.5K) using F-H for current and A-C for.
An Optimized Pupil Coronagraph: A New Way To Observe Extrasolar Planets This work was performed for the Jet Propulsion Laboratory, California Institute.
STUDY OF AMPLIFICATION ON ERBIUM DOPED FIBER AMPLIFIER Lita Rahmasari, Assoc. Prof. Dr. Yusof Munajat, Prof. Dr. Rosly Abdul Rahman Optoelectronics Laboratory,
Aim: How do we use SPSS to create and interpret scatterplots? SPSS Assignment 1 Due Friday 2/12.
Results Theory Abstract Evaluation of Scintillation Index and Intensity of Partially Coherent Laser Light MIDN 4/C Meredith L. Lipp and MIDN 4/C Kathryn.
Set-up for Levy Flight of Photons in Resonant Atomic Vapor Danielle Citro (SUNY Oswego), Adailton Feliciano (UFPB), Martine Chevrollier (UFPB), Marcos.
Physics 1809 Optics 3: Physical Optics Purpose of this Minilab Experiment with and learn about - Light intensity - Polarization - Diffraction - Interference.
ECE/ChE 4752: Microelectronics Processing Laboratory
Chapter 2 Basic Communication Theory Basic Communications Theory w Understand the basic transmission theory, and figure out the maximum data rate. w.
Static Pressure Control Loop The purpose of the static pressure control loop is to maintain an optimal static pressure in the ductwork. The control loop.
Detecting Electrons: CCD vs Film Practical CryoEM Course July 26, 2005 Christopher Booth.
ElectroScience Lab IGARSS 2011 Vancouver Jul 26th, 2011 Chun-Sik Chae and Joel T. Johnson ElectroScience Laboratory Department of Electrical and Computer.
National Center for Supercomputing Applications University of Illinois at Urbana-Champaign Image Features Kenton McHenry, Ph.D. Research Scientist.
Lesson 5 Conditioning the x-ray beam
ANATAC Meeting Line Length Correction Status 2004-Apr-23.
Acknowledgements References Conclusion Results Methods Introduction Analysis of Laser Light Propagation in a Maritime Environment Midshipman 1/C Daniel.
Telescope Technologies
Wireless and Mobile Computing Transmission Fundamentals Lecture 2.
ECEN 621, Prof. Xi Zhang ECEN “ Mobile Wireless Networking ” Course Materials: Papers, Reference Texts: Bertsekas/Gallager, Stuber, Stallings,
EELE 5490, Fall, 2009 Wireless Communications Ali S. Afana Department of Electrical Engineering Class 5 Dec. 4 th, 2009.
A deterministic source of entangled photons David Vitali, Giacomo Ciaramicoli, and Paolo Tombesi Dip. di Matematica e Fisica and Unità INFM, Università.
Transfer of Energy Through Water By: Sarah S Jessika F Nick L Halle B.
Overview Theory Index of Refraction and Path Length Setup and Procedure Michelson Interferometer Filming the Pressure Gauge Results Analysis Sources of.
Signals CY2G2/SE2A2 Information Theory and Signals Aims: To discuss further concepts in information theory and to introduce signal theory. Outcomes:
EE 6331, Spring, 2009 Advanced Telecommunication Zhu Han Department of Electrical and Computer Engineering Class 7 Feb. 10 th, 2009.
DECam Daily Flatfield Calibration DECam calibration workshop, TAMU April 20 th, 2009 Jean-Philippe Rheault, Texas A&M University.
11/23/2015Slide 1 Using a combination of tables and plots from SPSS plus spreadsheets from Excel, we will show the linkage between correlation and linear.
Double RF system at IUCF Shaoheng Wang 06/15/04. Contents 1.Introduction of Double RF System 2.Phase modulation  Single cavity case  Double cavity case.
SUBDIFFUSION OF BEAMS THROUGH INTERPLANETARY AND INTERSTELLAR MEDIA Aleksander Stanislavsky Institute of Radio Astronomy, 4 Chervonopraporna St., Kharkov.
MONALISA: The precision of absolute distance interferometry measurements Matthew Warden, Paul Coe, David Urner, Armin Reichold Photon 08, Edinburgh.
15. Fourier analysis techniques
Reza Malek-Madani Svetlana Avramov-Zamurovic Joe Watkins Will Peabody Andrew Browning United States Naval Academy Olga Korotkova University of Miami.
Joe Watkins Reza Malek-Madani Svetlana Avramov-Zamurovic Influence of wind shear on laser propagation.
Particle Image Velocimetry Demo Outline (For reference) ‏ Topic NumberTopic NamePage Type 1Flow of PIVAnimated page.
IPBSM Operation 11th ATF2 Project Meeting Jan. 14, 2011 SLAC National Accelerator Laboratory Menlo Park, California Y. Yamaguchi, M.Oroku, Jacqueline Yan.
Taikan SUEHARA, ATF2 meeting, KEK, 2006/11/22 Status of fringe stabilization of Shintake-monitor Taikan SUEHARA The University of Tokyo.
Michael Allen. MooSci  MooSci is a device that uses scintillation measurements from the Moon to reconstruct the ground layer turbulence profile.  This.
UBC/UW 2011 Hydrology and Water Resources Symposium Friday, September 30, 2011 DIAGNOSIS OF CHANGING COOL SEASON PRECIPITATION STATISTICS IN THE WESTERN.
RADAR ANTENNA. Functions of Radar Antenna Transducer. Concentrates the radiated energy in one direction (Gain). Collects echo energy scattered back to.
AirSpeed Calibration Facility by using LDV and A Wind Tunnel at CMS
Optical Characterization and Performances of Aerogel Radiator L.Barion, G.Battaglia, M. Contalbrigo, P. Lenisa, A.Movsisyan, L. Pappalardo, M. Turisini.
S. Rajbhandari, Z. Ghassemlooy, J. Perez, H. Le Minh, M. Ijaz,
Chapter 35-Diffraction Chapter 35 opener. Parallel coherent light from a laser, which acts as nearly a point source, illuminates these shears. Instead.
Interplanetary scintillation of strong sources during the descending phase near the minimum of 23 solar activity cycle Chashei I1., Glubokova1,2 S., Glyantsev1,2.
Optical PLL for homodyne detection
Kansas State University
Laser Beam Propagation in Maritime Environment
Complex Nanophotonics
Non-local Means Filtering
Meteorology & Air Pollution Dr. Wesam Al Madhoun
Presentation transcript:

Data Collection and Analysis Theory Motivation A Study of Propagation of Laser Light through a Turbulent Atmosphere MIDN 3/C Meredith L. Lipp Professor Svetlana Avramov-Zamurovic, Assistant Professor Charles Nelson The purpose of this project is to produce a method that will allow laser beams to propagate through a maritime environment with minimal scintillation (normalized variance to the mean intensity). This new technique could then be applied as a way to communicate over long distances with lasers rather than radio or as a weapon instead of missiles. Research in this area is being pursued fervently all around the country, and throughout the world as well. –Effected by turbulence: environmental effects that disrupt ideal light propagation and scatters it into a more disordered state. -Multi-Gaussian Schell Model (1) beam: varies from perfectly coherent to partially-spatially coherent. -Offsets effects of turbulence -Pseudo-partially spatially coherent beam (2): many realizations per data point should result in reduced scintillation -Physically unable to achieve what is required by theory at this point. The laser light was then propagated through the hot air turbulence emulator and recorded at the camera, which records at approximately 13 frames per second. Examples of the MATLAB produced screens for the SLM which determine the degree of coherence of the propagated beam. Methods Figure 1 Figure 1 shows the alignment of the laser, expander, and SLM. Hot Air Turbulence Emulator -Emulator: can be used to mimic some of the effects of high turbulence found by propagating a beam over a long distance. -Provides quick and easy control over turbulence strength -Statistically repeatable -Provides a random optical turbulence as compared with a static phase screen that is rotated and has a repeating phase pattern -Modular and extendable. Set up: -four heat guns providing thermal flow of 200 ̊ F -opposed by 4 fans providing ambient air counter flow. -heat from the guns is dispersed by three diffuser screens set in front of the heat guns. -Temperature probes spaced evenly throughout taking a reading every second. Previous analysis of these temperature changes categorized the turbulence as approximately Kolmogorov along the beam propagation axis with an average C n 2 value of 3.81E-11. (3) Laser Expander SLM Heat guns Temperature gauge Description of Equipment ThorLabs HNL020L nm Helium Neon Laser BNS Spatial Light Modulator (SLM) – XY Series ThorLabs DCU224M - CCD Camera 11 Amp Variable Temperature Heat Gun Thorlabs BEDS-10-A Expander Thermaltake Fans Omega 12 Channel Temperature Recorder RDXL 12SD This experiment’s goal was to examine the effects of pseudo-partially spatially coherent beams through turbulence. Ideally, the scintillation index would be minimized. However, initial results indicate that the scintillation was lower for all of the partially coherent beams. In addition, the pseudo- partially coherent beams had higher scintillation than the partially coherent beams through turbulence. This may be due to the fact that the SLM effected the pseudo-partially coherent beams when changing phase screens so rapidly. Further study will allow us to explore how to reduce scintillation using pseudo- partially coherent beams while maintaining intensity. Convolution and Fourier Transforms -Convolution: tool that produces the output of a system after passing a signal and noise through a specific filter. -Choosing a filter carefully can completely cancel the noise, producing only the desired signal -Fourier Transform: can be used to determine what will result from convoluting a filter and signal Conclusion Below is a graph of scintillation index versus coherence. When propagating beams, scintillation should be minimized. The data indicates that all but one of the partially coherent beams had a lower scintillation index than that of black. Black References (1)C. Nelson, S. Avramoz-Zamurovic, O. Korotkova, R. Malek-Madani, R. Sova, and F. Davidson. “Measurements of partially spatially coherent laser beam intensity fluctuations propagating through a hot-air turbulence emulator and comparison with both terrestrial and maritime environments.” (2)David Voelz and Kevin Fitzhenry. “Pseudo-partially coherent beam for free-space laser communication.” (3)C. Nelson. Experiments in Optimization of Free Space Optical Communication Links for Applications in a Maritime Environment,” dissertation from John Hopkins University, Process - Start camera and SLM - Warm up heat guns and fans - Begin temperature collection - Begin cycling - Begin camera recording Black (perfectly coherent) SLM Screen 2 (strong diffuser) SLM Screen 8 (weaker diffuser)