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Conference Abstracts and Presentations as Available
| Program Day |
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Program Session |
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| Invited Papers |
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|
Contributed Papers |
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| Day 1 - Monday July 9, 2007 |
| Session 1 |
Opening Session Fundamental Coherent Science and Technology |
|
Keynote Speaker, J. Hall, (JILA - University of Colorado and NIST),
Vibration-Resistant Laser Reference Cavity Design - A Highway to Optical Phase Stability and sub-Hz
Linewidth in the Real World
[Abstract1] [PowerPoint Presentation 1] [PowerPoint Presentation 2] |
|
M. Scully, (Texas A&M
University and Princeton University), The Photon: From the Quantum
Theory of Light to Vacuum Fuctuations and the Photon Wave Function |
|
P. Kumar, V. Grigoryan, (Northwestern University), and M. Vasilyev, (University of Texas at Arlington), Noise-Free Amplification: Towards Quantum Laser
Radar [PowerPoint Presentation] |
|
D. Payne, (Optoelectronics
Research Centre at the University of Southampton, UK), Kilowatt Fibre
Amplifiers as Highly Coherent Sources for Laser Radar [PowerPoint Presentation] [wmv Presentation] |
|
R.L. Byer (rlbyer@stanford.edu) and A. K.
Sridharan, (Stanford University), A Proposed
1-micron Eyesafe Lidar System for Global Space-based Remote Wind
Measurements
[Abstract2] [PowerPoint Presentation] |
| Session 2 |
Remote Sensing Priorities for the Future |
|
M.J. Kavaya, (NASA Langley), A Summary of the First Decadal Survey for Earth Sciences and Applications [PowerPoint Presentation] |
|
P. McManamon, (Air Force Research Laboratory), The Roles of Laser Radar
in Layered Sensing [PowerPoint Presentation] |
| Session 3A |
Ground and Airborne Wind Measurement Systems |
|
S.C. Tucker*, W.A. Brewer, R.M. Hardesty, S.P. Sandberg, A.M. Weickmann*,
D.C. Law, R.M. Marchbanks*, B.M. McCarty*, and J. Machol*, (NOAA Earth System
Research Laboratory), Ship-based High Resolution Doppler Lidar (HRDL)
Measurements of Boundary Layer Winds and Relative Aerosol Backscatter During
the 2006 Texas Air Quality Study (*Authors also with CU/CIRES)
[Abstract3] [PowerPoint Presentation] |
|
S. Rahm (stephan.rahm@dlr.de), I. Smalikho, and R. Simmet, (DLR, Germany), Recent Lidar-based Wake Vortex
Measurements at DLR
[Abstract4] [PowerPoint Presentation] [avi Presentation 1] [avi Presentation 2] [mpg Presentation] |
|
A. Adolfi-Bouteyre (adolfi@onera.fr), M. Valla, B. Augère, (ONERA, France), J.-P. Cariou, (ONERA and LEOSPHERE), D. Goular, D. Fleury, G. Canat, C. Planchat, T. Gaudo, L. Lombard, (ONERA, France), O. Petilon, and J. Lawson- Daku, (LEOSPHERE, France), 1.5 µm All Fiber Pulsed
Lidar for Wake Vortex Monitoring
[Abstract5] [paper] |
|
T. Ando (Ando.Toshiyuki@ap.Mitsubishi Electric.co.jp), S. Kameyama, T. Sakimura, K. Asaka, and Y. Hirano, (Mitsubishi Electric Corporation, Japan)
[Abstract6] |
|
J.P. Cariou (jpcariou@leosphere.fr), (LEOSPHERE, France), R. Parmentier, (LEOSPHERE, France), M. Valla, (ONERA, France), L. Sauvage, (LEOSPHERE, France), I. Antoniou, (Risø, Wind Energy Department, Denmark), and M. Courtney (Risř, Wind Energy Department, Denmark), An Innovative and Autonomous 1.5 µm
Coherent Lidar for PBL Wind Profiling
[Abstract7] [PowerPoint Presentation] |
|
R. Frehlich (rgf@cires.colorado.edu), Y. Miellier, and M.L. Jensen, (University of Colorado), Coherent Doppler Lidar
Measurements of the Atmospheric Boundary Layer
[Abstract10] [PowerPoint Presentation] |
| DAY 2 - Tuesday, July 10, 2007 |
| Session 3B |
Ground and Airborne Wind Measurement Systems (Continued) |
|
J. Mann, T. Mikkelsen, I. Antoniou, M. Courtney, F. Bingöl,
G. Larsen, and H.E. Jřrgensen, (Risř National
Laboratory at the Danish Technical University, Denmark), Lidars in Wind
Energy [PowerPoint Presentation] [avi Presentation] |
|
K. Mizutani, T. Itabe, S. Ishii, T. Aoki, Y. Murayama, H. Iwai, (National Institute of
Information and Communication Technology, Japan), K. Asai, A. Sato, (Tohoku Institute of Technology, Japan), H. Fukuoka, (Hamamatsu Photonics K.K., Japan), and T. Ishikawa, (Nippo Aleph Co., Japan), Wind Lidar
Developments and Measurements at NICT
[Abstract11] [PowerPoint Presentation] |
|
A. Linganagari (alingana@asu.edu), R. Calhoun, and H.J.S Fernando, (Arizona State University). Analysis of the
Nocturnal Development and Dispersion of Smoke Puffs in the Atmosphere using
Lidar
[Abstract12] [PowerPoint Presentation] [mpg Presentation-Front View] |
|
Y.L. Pichugina (yelena.pichugina@noaa.gov), (Cooperative Institute for Research in Environmental Sciences (CIRES) and NOAA Earth System Research Laboratory (ESRL)), R.M. Banta, (NOAA Earth System Research Laboratory (ESRL)), N.D. Kelley, B.J. Jonkman, (National Wind Technology Center/National Renewable Energy Laboratory), W.A. Brewer, S.P. Sandberg, (NOAA Earth System Research Laboratory (ESRL)), and J.L. Machol, (Cooperative Institute for Research in Environmental Sciences (CIRES) and NOAA Earth System Research Laboratory (ESRL)), Advantage of
the High Resolution Doppler Lidar Measurements for Nighttime PBL Study and
Wind-energy Applications
[Abstract13] [PowerPoint Presentation] |
|
S.M. Hannon (steve.hannon@lmct.com), S.R. Vetorino and J.V. Pelk, (Lockheed Martin
Coherent Technologies), Next Generation Doppler
Lidar Sensor at 1.6 microns
[Abstract14] [pdf Presentation] |
|
D. Emmitt (gde@swa.com) and C. O’Handley, (Simpson
Weather Associates), Airborne Doppler Wind Lidar Prospecting for Vertical Structures
at Flight Level
[Abstract59] [PowerPoint Presentation] |
|
M.J. Kavaya (michael.j.kavaya@nasa.gov), F. Amzajerdian, G.J. Koch, U.N. Singh, and J. Yu, (NASA Langley
Research Center), Coherent Lidar Activities
at NASA Langley Research Center
[Abstract15] [PowerPoint Presentation] |
|
N. Schmitt (nikolaus.schmitt@eads.net), W. Rehm, T. Pistner, H. Diehl, P. Navé, (EADS Innovation Works, Germany), G. Jenaro-Rabadan, P. Mirand, and M. Reymond, (AIRBUS SAS, France), Flight of the Awiator Airborne LIDAR
Turbulence Sensor - Final Results
[Abstract16] [pdf Presentation] |
|
M. Valla, C. Planchat, L. Lombard, D. Goular, T. Gaudo, D. Fleury, A. Dolfi-Bouteyre, G. Canat , C. Besson, B. Augčre, (ONERA)
J.P. Cariou, J. Lawson, O. Petilon, (Leosphere),
Pulsed Fibre Lidar for Wake Vortex Monitoring [PowerPoint Presentation] |
| Session 4 |
Space-Based Lidar |
|
H. Nett (herbert.nett@esa.int) and M. Endeman,
(European Space Agency, ESTEC), ADM-Aeolus Mission: Operation and Data
Processing
[Abstract17] [PowerPoint Presentation] |
|
Y. Durand (yannig.durand@esa.int), A. Héličre, P. Bensi, J.-L. Bézy, and
R. Meynart, (European Space Agency, Earth Observation Projects), Lidars in
ESA's Earth Observation Missions
[Abstract18] [PowerPoint Presentation] |
|
A. Dabas (alain.dabas@meteo.fr), M.-L. Denneulin, (Météo-France, Centre National de Recherches Météorologiques, France), P. Flamant, (Centre National de la recherché Scientifique, Laboratoire de Météorologie Dynamique, France), O. Reitebuch,
J. Streicher, I. Leike, D. Huber, and U. Paffrath, (Deutsches Zentrum für Luft und Raumfahrt, Institut für Physik der Atmosphäre, Germany),
Wind Retrieval from ADM-Aeolus Signals
[Abstract19] [PowerPoint Presentation] |
|
M.-L. Denneulin (marie-laure.denneulin@cnrm.meteo.fr), (Météo-France/CNRS, CNRM/GAME, France), P. Flamant, J. Cuesta, (Centre National de la Recherche scientifique, Laboratoire de Météorologie Dynamique, Institut Pierre Simon, France), A. Dabas, (Météo-France/CNRS, CNRM/GAME, France), and D. Huber, (DLR, Germany),
ADM-Aeolus Spin-off Products and Retrieval Algorithms
[Abstract20] [PowerPoint Presentation] |
|
Y. Durand (yannig.durand@esa.int), A. Hélière, J.-L. Bézy, and R. Meynart, (European Space Agency, Earth Observation
Projects), Lidar Technology Developments for ESA's Earth Observation Missions
[Abstract21] [PowerPoint Presentation] |
|
C. Grund (cgrund@ball.com),
M. Stephens, and C. Weimer, (Ball Aerospace & Technologies Corporation), Optical
Autocovariance Wind Lidar and Performance from LEO
[Abstract22] [PowerPoint Presentation] |
|
M.J. Kavaya (michael.j.kavaya@nasa.gov) and R.G. Frehlich, (NASA Langley Research Center), Lidar and Mission Parameter
Trade Study of Space-Based Coherent Wind Measurement Centered on NASA’s 2006
GWOS Wind Mission Study Parameters
[Abstract24] [PowerPoint Presentation] |
|
B. Gentry, M. Magill, J. Corner, and G. Schwemmer, (NASA Goddard Space
Flight Center), Direct Detection Doppler Lidar Development at NASA's
Goddard Space Flight Center: Past, Present, and Future [pdf Presentation] |
|
D. Winker and Y. Hu, (NASA
Langley Research Center), The CALIPSO Mission and Initial Inputs for
Doppler Wind Lidar Studies
[Abstract25] |
| Session 5 |
CO2 Measurement Lidar
|
|
J.B. Abshire, H. Riris, R. Kawa, X. Sun, M.A. Krainak, J.-P. Mao, G.J. Collatz, M.A. Stephen, J. Chen, E. Wilson, (NASA Goddard
Space Flight Center), Laser Sounder for Remote Measurements of CO2
Concentrations in the Troposphere [PowerPoint Presentation] |
|
G. Spiers, (NASA Jet Propulsion
Laboratory), Recent Results and Progress on the Development of a Laser
Absorption Spectrometer for Carbon Dioxide Sink and Source Detection [PowerPoint Presentation] |
| Session 12 |
Poster Session |
| POSTER |
V. Banakh (banakh@iao.ru),
D.A. Marakasov, (Institute of Atmospheric Optics SB RAS, Russia), and M.A. Vorontsov (U.S. Army Research Laboratory), Reconstruction of
Cross-wind Profile From Turbulent Intensity Fluctuations of Diffusely
Scattered Optical Wave
[Abstract56] [paper] |
| POSTER |
G. Busch, and D.F. Pierrottet, (Coherent
Applications, Inc.), Dispelling the Myth of Reduced Heterodyne
Efficiency With Increasing Detection Aperture
[Abstract57] [paper] |
| POSTER |
K.M. Kwong (Hong Kong Polytechnic University, China) and P.W. Chan, (Hong Kong Observatory, China), LIDAR-based Turbulence Intensity Calculation along
Glide Paths
[Abstract58] [paper] |
| POSTER |
D. Emmitt (gde@swa.com) and S.Greco, (Simpson
Weather Associates), CFLOS Statistics for Design of Future Space Based Lidars
[Abstract23] [paper] |
| POSTER |
P. Gatt (phil.gatt@lmco.com)
and S. Shald, (Lockheed Martin Coherent Technologies), Coherent Ladar Angle Estimation
Error Analysis
[Abstract60] [paper] |
| POSTER |
H. Iwai (iwai@nict.go.jp),
S. Ishii, K. Mizutani, Y. Murayama, (National Institute of Information and Communications Technology, Japan), N. Kaku, (Electronic Navigation Research Institute, Japan), S. Weiming, T. Yamazaki, and T. Iwasaki, (Department of Geophysics, Tohoku University, Japan), Single-
and Dual-lidar measurements of the sea breeze at Ssendai Airport
[Abstract68] [paper] |
| POSTER |
J.W. Katz (j-katz@tamu.edu), (Texas A&M University),
Laboratory Development of
a Brillouin LIDAR Using Edge-Filter Detection for Measurement of Sound
Velocity in the Ocean
[Abstract61] |
| POSTER |
K.T. Lowe (toddlowe@aurinc.com) and R.L. Simpson, (Applied University Research, Inc.), Doppler Chirp
Signal Processing for Particle Acceleration Measurement with Laser-Doppler
Velocimetry
[Abstract67] |
| POSTER |
J. Mason (james.e.mason@lmco.com), J.E. Mann, K.A. Anderson, R.L. Kendrick, T.S. Kubo, J. C. Marron, and T. Zhao, (Lockheed Martin Advanced Technology Center),
Experiments with Multi-Aperture Three Dimensional Coherent
Imaging
[Abstract62] |
| POSTER |
C. Roychoudhuri, (University of Connecticut) and N.S. Prasad (n.s.prasad@larc.nasa.gov), (NASA Langley
Research Center), A Deeper Look
at the Fundamentals of Heterodyne Detection Requirements
[Abstract63] [paper] |
| POSTER |
S. Serati (sserati@bnonlinear.com) and J. Stockley, (Boulder Nonlinear Systems, Inc.), Dynamic
Holographic Beam Steering |
| POSTER |
S. Shald, (scott.shald@lmco.com), (Lockheed Martin), Comparison of FIR and IIR
Filters in Coherent Lidar Processing
[Abstract64] [paper] |
| POSTER |
I. Shpantzer, P. Cho (pscho@celight.com), (CeLight, Inc.), J. Khurgin, (Johns Hopkins University), A Novel Coherent Laser Radar Architecture Based on
Temporal-diversified Optical Orthogonal-frequency-division-multiplexing
[Abstract70] [paper] |
| POSTER |
D.G.H. Tan (david.tan@ecmwf.int), E. Andersson, J. de Kloe, G.-J. Marseille, A. Stoffelen, P. Poli, M.-L. Denneulin, A. Dabas, D. Huber, O. Reitebuch, P. Flamant, O. Le Rille, A.-G. Straume, and H. Nett, (ECMWF), ADAM-Aeolus Level-2B Wind Retrieval Algorithms
[Abstract65] [PowerPoint Presentation] |
| POSTER |
R.J. Hill, A. Brewer, and S.C. Tucker, (sara.tucker@noaa.gov), Cooperative Institute for Research in the Environmental Sciences, University of Colorado and Earth Systems Research Laboratory, NOAA,
Platform-Motion Compensation for Velocity Measured by Doppler Lidar [paper] |
| POSTER |
N. Tsunematsu (n.tsunematsu@nict.go.jp), H. Iwai, S. Ishii, Y. Murayama, M. Yasui, K. Mizutani, S. Kawamura, and Y. Ohno, (National Institute of Information and
Communications Technology (NICT)), A Case Study of Multi-layered Wind
Structure Over Tokyo Associated With Sea Breeze Circulation by Use of a
Coherent Doppler Lidar and the WRF Model
[Abstract69] [paper] |
| POSTER |
D. Youmans (DYoumans@sparta.com), (SPARTA, Inc.), Range-Doppler Imaging Using
Pseudo-Random Phase Modulation Coherent Ladar: A Study Using the SEASAT
Satellite Retro-Reflectors
[Abstract66] [PowerPoint Presentation] |
| DAY 3 - Wednesday, July 11, 2007
|
Session 5
|
CO2 Measurement Lidar (Continued)
|
|
P. Flamant, (Ecole
Polytechnique, France), Road to CO2 DIAL Mission [PowerPoint Presentation] |
|
M. Dobbs, W. Sharp,
J. Jenney, (ITT Space Systems), Method and Performance of Modulated-CW Lidar for
Mapping Sources and Sinks of Carbon Dioxide
[Abstract26] [PowerPoint Presentation] |
|
F. Gibert (fabien.gibert@lmd.polytechnique.fr), ( Ecole Polytechnique, France), L. Joly, (GSMA, Université de Reims), I. Xueref-Remy, M. Schmidt, M. Ramonet, (IPSL-LSCE), P.H. Flamant, (Ecole Polytechnique, France), D. Bruneau, (IPSL-SA, Université Pierre et Marie Curie), and D. Edouart, (Ecole Polytechnique, France),
2-µm Heterodyne DIfferential Absorption Lidar
for Both Atmospheric CO2 and Wind Measurements: Validation and Geophysical
Application
[Abstract27] [PowerPoint Presentation] |
|
S. Ishii (sishii@nict.go.jp),
K. Mizutani, T. Itabe, T. Aoki, (National Institute of Information and Communications Technology, Japan), K.Asai, and A. Sato, (Tohoku Institute of Technology, Japan), Coherent Differential Absorption Lidar for atmospheric CO2
Measurement
[Abstract28] [PowerPoint Presentation] |
|
S. Kameyama, (Kameyama.Shumpei@dn.MitsubishiElectric.co.jp), S. Ueno, Y. Hirano, N. Sugimoto, and T. Kimmura, (Mitsubishi Electric
Corporation, Japan)
[Abstract29] |
| Session 6 |
Hard Target Laser Radar |
|
J.M. Sabatier, (University of
Mississippi) and V. Aranchuk, (Metrolaser, Inc.), Multiple Beam Laser
Doppler Vibrometry for Landmine Detection
[Abstract30] [PowerPoint Presentation] [mpg Presentation] |
|
O. Steinvall, (Swedish Defence Research Agency (FOI), Sweden),
Recent Lidar Developments at FOI
[Abstract31] [pdf Presentation] |
|
M. Vaidyanathan, S. Blask,
and V. Reynolds, (Harris Corporation) and R. Marino, (MIT Lincoln Laboratory),
Field Demonstration of 3-D Photon Counting Lidar for Imaging Through
Foliage |
|
J. Buck (joe.buck@lmco.com), A. Malm, A. Zakel, B. Krause, and B. Tiemann, (Lockheed Martin),
S3 Program Update: High-Resolution
Three-dimensional Imaging
[Abstract32] [PowerPoint Presentation] [avi Presentation - Outdoor Jeep Camo Single Shot] [avi Presentation-Outdoor Jeep] [avi Presentation-Average White Dots] [avi Presentation-Intensity Dots] |
|
D. Jameson (Douglas.Jameson@wpafb.af.mil), M. Dierking, (Air Force Research Laboratory) and B. Duncan, (Electro Optics Program, University of Dayton), Effects of Spatial Averaging on Coherent Ladar Pulse-Pair
Vibration Measurements
[Abstract33] [PowerPoint Presentation] |
| DAY 4 - Thursday, July 12, 2007
|
| Session 7 |
Modeling and Simulation |
|
A. Belmonte (belmonte@tsc.upc.edu), (Technical
University of Catalonia, Spain), Atmospheric Aberrations in
Coherent Laser Systems
[Abstract34] [PowerPoint Presentation] |
|
D. Jacob (don.jacob@lmco.com)
and P. Gatt, ( Lockheed Martin Coherent Technologies), Coherent Lidar CNR: A Summary of
the Effects of Refractive Turbulence and the Dependence on the Normalized
Irradiance Variance
[Abstract35] [PowerPoint Presentation] |
|
P. Gatt (phil.gatt@lmco.com),
T. Nichols, and S. Johnson, (Lockheed Martinolo Coherent Techngies), Finite Dead-Time Geiger-Mode APD
Performance
[Abstract36] [pdf Presentation] |
|
M.A. Greiner (Greiner@wpafb.af.mil),
D. Bradley, D. Duncan, and M.P. Dierking, (University of Dayton), Monte Carlo Canopy
Propagation Model
[Abstract37] [PowerPoint Presentation] |
| Session 8 |
Related Coherent Optical Technologies and Applications |
|
M.G. Taylor, (Atlantic Sciences), Coherent Detection for Fiber Optic Communications Using
Real Time Digitial Signal Processing
[Abstract38] [PowerPoint Presentation] |
|
V. Quetschke, (LIGO
Scientific Collaboration, University of Florida), LIGO - Coherent Optical
Length Measurement with 10-18 m Accuracy
[Abstract39] [PowerPoint Presentation] |
|
B. Smutny, R. Lange, G. Mühlnikel, and F. Heine, (Tesat-Spacecom GmbH
& Co.KG, Germany), Coherent Laser Communications Terminals for
LEO-GEO Data Links
[Abstract40] [pdf Presentation] |
| Session 9 |
Synthetic and MultiAperture Coherent Laser Radar Systems |
|
J. Ricklin, B. Schumm, and P. Tomlinson, (DARPA), Synthetic Aperture Ladar for
Tactical Imaging (SALTI) Flight Test Results and Path Forward
[Abstract41] [PowerPoint Presentation] |
|
J.C. Marron
(joe.marron@lmco.com), R.L. Kendrick, T.A. Höft, and N. Seldomridge, (Lockheed Martin Coherent Technologies), Novel
Multiaperture 3D Imaging Systems
[Abstract42] [PowerPoint Presentation] |
|
N.J. Miller, (University of Dayton), M.P. Dierking, (Air Force Research Laboratory), and B.D.
Duncan, (University of Dayton), Sparse Aperture Imaging
[Abstract43] [PowerPoint Presentation] |
| Session 10A |
Novel Systems |
|
Mark Rubin (rubin@LL.mit.edu) and S. Kaushik,
(MIT Lincoln Laboratories), Quantum States and Coherent Laser Radar [PowerPoint Presentation] |
|
J. Ashcomb, S. Kaushik, R.M. Heinrichs, (MIT Lincoln
Laboratories), Coherent Detection with Photon Counting Receivers
[Abstract45] [PowerPoint Presentation] [avi Presentation] |
|
N. Newbury, W.C. Swann, and I. Coddington, (National Institute
of Standards and Technology), Lidar with Femtosecond
Fiber-Laser Frequency Combs
[Abstract46] [PowerPoint Presentation] |
|
R. Babbitt, P.A. Roos, Z. Cole, R.R. Reibel, T. Berg, B. Kaylor, K.D. Merkel, K.H. Wagner, F. Schlottau, Y. Li, and A. Hoskins, (Montana State
University), High Resolution Range/Doppler Ladar Using Broadband
Coherent Optical Processing [PowerPoint Presentation] |
|
S.L. Jain (sljain@nplindia.ernet.in), (National Physical Laboratory),
[Abstract48] [PowerPoint Presentation] |
|
P. Lindelow
(pli@oersted.dtu.dk), (Orsted-DTU, COM/DTU, Technical University of Denmark, Denmark),
Velocity Sensing FSPT-Modulated Coherent Lidar [PowerPoint Presentation] |
| DAY 5 - Friday, July 13, 2007
|
| Session 10B |
Novel Systems (Continued) |
|
| J.C. Chen (jcchen@ll.mit.edu) and S. Kaushik, (MIT Lincoln
Laboratory), Terahertz Vibrometer that Senses
Sub-micron Vibrations Behind Barriers
[Abstract47] [paper] |
|
M.J. Khan (mjkhan@ll.mit.edu),
J.C. Chen, and S. Kaushik, (MIT Lincoln Laboratory), Optical Detection of Terahertz Using Nonlinear
Parametric Upconversion
[Abstract49] [PowerPoint Presentation] |
| Session 11 |
Advanced Component Technologies |
|
F. Amjajerdian, B.L. Meadows, N.R. Baker, B.W. Barnes, U.N. Singh, and M.J. Kavaya, (NASA Langley
Research Center), Qualification Testing of Laser Diode Pump Arrays
for a Space-based 2-micron Coherent Doppler Lidar
[Abstract50] [PowerPoint Presentation] |
|
Mike Salisbury, J. Boisvert, S. Connors, G. Stuart, and A. Portillo, (Boeing SVS),
Geiger Mode Array Tech Transfer and Terrain Mapping Data
Collection
[Abstract51] [PowerPoint Presentation] [avi Presentation] |
|
F. Hovis, (Fibertek, Inc.), C. Weimer, J. Applegate, (Ball Aerospace & Technologies Corp.), A. Cook, J. Hair, (NASA Langley Research Center), B. Gentry, (NASA Goddard Space Flight Center), J. Wang, (Raytheon Space and Airborne Systems), and M. Dehring, (Michigan Aerospace Corp.),
Advanced Transmitters for Ladar Applications
[Abstract52] [pdf Presentation] |
|
D. Edouart (edouart@lmd.polytechnique.fr) and P.H. Flamant, (IPSL-LMD, Ecole Polytechnique), Using a Photo-acoustic Cell
to Manage Pulsed Laser Spectral Shift: Application to Accurate Atmospheric
CO2 Heterodyne Differential Absorption Lidar Measurements
[Abstract53] [PowerPoint Presentation] |
|
F. Heine (frank.heine@tesat.de) and
R. Lange, (Tesat-Spacecom GmbH & Co.KG),
[Abstract54] [pdf Presentation] |
|
B. Stoneman (bob.stoneman@lmco.com), R. Hartman, E.A. Schneider, A.I.R. Malm, S.R. Vetorino,
C.G. Garvin, J.V. Pelk, S.M. Hannon, and S.W. Henderson, (Lockheed Martin Coherent Technologies), Eyesafe 1.6 Micron Er:YAG
Transmitters for Coherent Laser Radar
[Abstract55] [pdf Presentation] |
[1]
While
heterodyne laser techniques offer remarkable sensitivity in principle,
experimental results are usually seriously compromised by environmental
vibration. Accordingly, much attention has been invested on reducing the
vibration amplitude experienced by the stable cavity being used for laser
frequency control. We have recently shown it is valuable to reduce the
intrinsic vibration sensitivity of the cavity itself, which is easily achieved
using symmetry suitably in the cavity mounting. At present, sub-Hz optical
linewidths are easily demonstrated in an ordinary laboratory, with the present
limitation ~0.3 Hz being fixed by thermal noise of the mirror’s coated surface.
Frequency drift rates can be <20 milliHz/s.
[2]
This
paper will review the history and progress and the challenge of global remote
sensing of wind with an emphasis on solid state laser transmitter development.
We reconsider the long-standing notion that transmitter wavelengths greater
than 1.4 microns are necessary for eye-safe operation. We present a design for
a satellite based lidar system that meets the NASA specifications for eyesafe
global wind sensing and operates using the well developed 1 micron laser
technology.
[3]
The
NOAA Earth System Research Laboratory has two coherent Doppler lidar systems
that have been deployed onboard research vessels during several experiments.
Those instruments measure the wind velocity relative to the motion of the
lidar. The correction for the motion of the platform is is derived and
implemented. The analysis is general enough to be applied to Doppler velocity
measurements from all monostatic ship- and aircraft-borne lidars and radars,
and generalization to bistatic systems is doable. The correction is
demonstrated using mini-MOPA Doppler velocity data obtained during the Rain In
Cumulus over the Ocean (RICO) experiment.
[4]
In
the last two years several ground based and airborne wake vortex campaigns have
been performed with the DLR coherent Doppler Lidar. The objective of those
campaigns was the measurement and description of the wakes generated by the new
Airbus A380 aircraft for the ICAO landing separation as well as the influence
of different configurations on the vortex life time in the project
AWIATOR.
[5]
A
new 1.5 µm pulsed Lidar using an all fiber laser source has been developed by
ONERA in cooperation with Leosphere , for wake vortex and wind field
measurements . This paper illustrates the good results obtained with a pulsed
lidar based on MOPFA 1.5µm laser, for detection and monitoring of wake vortices
on airport fields. Operational ranges larger than 400m have been demonstrated,
with a 60µJ, 15kHz, 250ns pulse fiber doped Er laser. Wake profiles, positions
and circulations can be derived from recorded data.
[6]
Long
range all-fiber Coherent Doppler LIDAR (CDL) system has been developed for wind
sensing. A newly developed Er3+/Yb3+ fiber MOPA (Master Oscillator Power
Amplification) source has enabled transmitting optical pulse to be performed
its pulse energy of several tenth micro joule, which was previously limited up
to several micro joule because of Stimulated Brillouin Scattering (SBS) in an
optical fiber. The new all-fiber CDL has successfully measured maximum range
for wind velocities up to 8km which is about 5 times as long as the measurable
distance of a few kilometer in a conventional all-fiber CDL.
[7]
The “EZ WIND LIDAR”TM is a coherent wind lidar developed by LEOSPHERE taking
into account the ONERA’s advance in heterodyne lidar and fiber laser
technology. This eye safe non visible and soundless, robust, easily portable,
low consumption system is dedicated to horizontal and vertical wind speed and
direction profiles measurements at altitudes from 45 to 200m. We describe in
this paper the main characteristics of the system, the post processing we have
developed, and the first results of an independent validation campaign at the
RISOE test bed in Denmark in spring 2007.
[8]
This
paper discusses the application of 4DVAR technique to analyze the
terrain-disrupted airflow at the Hong Kong International Airport based on LIDAR
data. The conical scans of the LIDAR are employed in the study. The analyzed
wind field is found to reveal many salient features of the terrain-induced
disturbances, such as mountain wave and jump-like feature in the gap flow in
stable boundary layer. It could be useful in the day-to-day monitoring of the
airflow at the airport area.
[9]
The
Hong Kong Observatory develops the automatic LIDAR-based Windshear Alerting
System (LIWAS) for the Hong Kong International Airport. This paper discusses a
refinement of the method to better capture windshear in rapidly fluctutaing
wind condition, such as terrain-disrupted airflow. The method is found to
outperform the original LIWAS algorithm by 10-30% in terms of the hit rate of
windshear, with a modest increase of alert duration.
[10]
Coherent
Doppler lidar derived profiles of wind and turbulence are presented for various scanning and processing techniques and compared with high
resolution in situ measurements of small scale turbulence. Simultaneous estimates of
the energy dissipation rate, velocity variance, and outer scale of
turbulence are produced for the two orthogonal horizontal velocity components
(longitudinal and transverse). The impact of filtering the radial velocity data to remove
the large scale atmospheric processes from the small scale turbulence is
presented. Critical lidar engineering design and scanning issues are identified for the
challenging conditions of low turbulence.
[11]
NICT
is conducting research of coherent Doppler lidars for 'Sensing Network
Project' and space based wind profiling. 2micron Q-switched output of 100mJ at
20Hz has been achieved in a Tm,Ho:YLF laser oscillator for ground based wind
profiling and CO2 measurement. The experiments show that very good thermal
conduction is held between rod and heat sink. Another type of Tm,Ho:YLF laser
oscillator with 50-100mJ output at 20-30Hz will be developed for coherent
Doppler lidars. The coherent Doppler lidars with moderate output laser will be
used in the Sensing Network Project, where wind inforrmation obtained with a
group of instruments over the area around Tokyo should be collected through
network.
[12]
An
atmospheric dispersion study was conducted in Oklahoma City, Oklahoma, in July
2003 during the Joint Urban study. On the night of July 4th, the ASU and ARL
lidars performed a set of complementary scans in region east of the CBD
(Central Business District) to capture the aerial movement and dispersion of
smoke puffs from the fireworks display. The ASU lidar was located at the
south-east side of the CBD and ARL lidar was located towards the north-east.
The purpose of this study was to use the data collected from those scans to
capture the puff’s movement, shape, and size development as it advects in the
atmosphere. We present a methodology for measuring dispersion parameters based
on lidar images, which can be used effectively to monitor the time variations
of the puff and to deduce its dispersion parameters downstream. The lidars used
by ASU and ARL for performing the corresponding scans and collecting the
required data were Coherent Doppler lidar.
[13]
The
High-Resolution Doppler Lidar has been highly effective in the study of dynamic
processes in the atmospheric boundary layer (ABL) because of its temporal and
spatial resolution. Recently applications involving wind energy have become
important, because accelerated flows occurring at night in the form of
low-level jets (LLJs) have proven to be an important resource over the U.S.
Great Plains. In this paper we will describe the role of the nocturnal LLJ in
generating turbulence and turbulent fluxes, and we show the advantages of lidar
data for wind–energy applications
[14]
We
report on work to develop a pulsed coherent Doppler lidar operating at 1.6
microns using a novel ‘laser pumping a laser’ architecture. This system
provides higher average power, roughly half the pulse duration, a higher and
adaptable PRF, and significantly smaller size, weight and power consumption as
compared with the existing 2 micron WindTracer® system. Additional related
developments have enhanced the signal processor and super-hemispherical
scanner, plus overall reliability, supportability, and performance have been
enhanced. Key features are described and sample performance results are
provided.
[15]
NASA
Langley Research Center has been developing and using coherent lidar systems
for many years. The current projects at LaRC are the Global Wind Observing
Sounder (GWOS) mission preparation, the Laser Risk Reduction Program (LRRP),
the Instrument Incubator Program (IIP) rugged wind lidar project, the
Autonomous Landing and Hazard Avoidance Technology (ALHAT) project for lunar
landing, and the Skywalker project to find and use thermals to extend UAV
flight time. These five projects encompass coherent lidar technology
development, characterization/validation/calibration facilities, computer
simulation, compact/rugged packaging, trade studies, data
acquisition/processing/display, system demonstration, and mission design. This
paper will further discuss these activities at LaRC.
[16]
First
flight test results of the AWIATOR airborne direct detection UV LIDAR for
turbulence sensing are presented. The sensor was installed in an Airbus A340
aircraft in a fairing below the aircraft nose and measured in four directions
ahead at >= 50m distance in order to determine the 3D wind vector. Good
Rayleigh signals could be gathered even in flight altitudes up to 39.00 ft in
clear, aerosol depleted air. Line-of-sight standard variations of the measured
speed was around 1.6 m/s at that maximum altitude. First results show good
follow-up of the LIDAR data to the aircraft onboard TAS sensor.
[17]
The
Atmospheric Dynamics Mission (ADM-Aeolus) is the second core mission within
ESA's Earth Explorer Programme. Planned for launch in 2009 Aeolus will deliver
global wind observations throughout a planned lifetime of 3 years, serving both
numerical weather prediction and various scientific applications.
Aeolus' payload ALADIN is a direct detection Doppler Lidar operating in the
ultraviolet. Equipped with a dual-channel receiver system it will allow
independent detection of the aerosol and molecular components of the
atmospheric backscatter signal, covering a height range from 0-25 km. An
outline will be given on the spacecraft and payload design and on the ground
segment concept.
[18]
Spaceborne
lidars have been the subject of extensive investigations by the European Space
Agency since the mid 1970’s, resulting in mission and instrument concepts, such
as ATLID, the ATmospheric backscatter LIDar payload of the EarthCARE (Earth
Clouds, Aerosols, and Radiation Explorer) mission, ALADIN, the Doppler Wind
Lidar of the ADM-Aeolus mission (Atmospheric Dynamics Mission), a water vapour
Differential Absorption Lidar considered for the WALES mission (Water Vapour
Lidar Experiment in Space) and more recently a CO2 Total Column Differential
Absorption Lidar considered for the A-SCOPE mission (Advanced Space Carbon and
Climate Observation of Planet Earth). These studies have shown the basic
scientific and technical feasibility of spaceborne lidars, but they have also
demonstrated their instrumental complexity.
As a result, the Agency undertook technology developments in order to
strengthen the instrument maturity. The purpose of this paper is to present the
technology and instrument developments that are currently running at the ESA in
support to EarthCARE, the 6th selected Earth Explorer mission, and to A-SCOPE,
a candidate mission for the 7th Earth Explorer mission. The pre-development
activities span over a broad range addressing all the critical stages from the
transmitter to the receiver and covering both components development and
characterisation and sub-systems development
[19]
The
direct-detection wind lidar mission ADM-Aeolus of the European Space Agency
implements two detection channels, one for molecules and one for particles. The
molecular channel is based on dual Fabry-Perot. The inversion of the response
must be corrected from pressure and temperature effects. The Mie channel is
based on a fringe imaging technique using a Fizeau interferometer. The fringe
is sampled by a 16-element CCD. The processing of the 16 photocounts aims at
estimating the central frequency of the fringe. The algorithm is presented and
compared to techniques currently used for heterordyne lidars.
[20]
The
Atmospheric Dynamic Mission ADM-Aeolus has the objective to measure wind
profiles from space using a Lidar operating in the UV. Based on a dual-channel
design that allow the detection of molecular and particulate signal, ADM-Aeolus
is a High Sprectral Resolution Lidar. It enables the retrieval of cloud and
aerosol layers optical properties as spin-off products. This paper presents the
basic concept of the L2A processor , responsible for this task. Some solutions
are proposed to answer to identified problems due to accumulation of signals in
range bins. Some preliminary numerical testing has been conducted and first
results are presented.
[21]
The
idea of deploying a lidar on an Earth-orbiting satellite stems from the need
for continuously providing profiles of atmospheric structure with high
accuracy, resolution and global coverage independently of the lighting
conditions. Interest in this information for climatology, meteorology and the
atmospheric sciences in general is huge. Areas of application range from the
determination of global warming and greenhouse effects, to monitoring the
transport and accumulation of pollutants in different atmospheric regions, to
the assessment of the largely unknown microphysical properties and the
structural dynamics of the atmosphere itself.
Spaceborne lidar systems have been the subject of extensive investigations by
the European Space Agency since the mid 1970’s, resulting in two Earth Explorer
missions approved for flight: ADM-Aeolus (Atmospheric Dynamics Mission) and
EarthCARE (Earth Clouds, Aerosols, and Radiation Explorer); one mission studied
up to Phase A: WALES (Water Vapour Lidar Experiment in Space) and one mission
recently selected as a candidate for the 7th Earth Explorer mission: A-SCOPE
(Advanced Space Carbon and Climate Observation of Planet Earth). The purpose of
this paper is to present both approved and currently studied missions and their
related instruments concept, all relying on different use of lidar.
[22]
The
Optical Autocovariance Wind Lidar (OAWL) direct detection interferometric
technique promises to provide the aerosol sensitivity of a coherent system
while also measuring winds from molecular backscatter. The OAWL method has the
advantages of being insensitive to aerosol to molecular backscatter mixing
ratio, requiring no absolute wavelength control, no receiver to transmitter
relative frequency control, no injection seeding control loops, and no tuning
for spacecraft velocity compensation. OAWL has recently been demonstrated at
Ball. This paper discusses the theory, proof of concept test results, and
anticipated performance from LEO.
[23]
Lidars
in space such as LITE, GLAS and more recently CALIPSO provide laser beam scale
statistics on cloud penetration and contiguous cloud free scenes. For those
lidars (e.g. coherent DWL) probing the lower troposphere through partly cloudy
areas, understanding cloud porosity is critical to the design of the sampling
pattern. For lidars whose accuracy scales directly to the number of photons
detected and whose signal may be compromised by a small cloud in the
integration window (e.g. integration on a chip), knowing the probability of
cloud free intervals is important in performing system trades.
This paper will summarize a study completed for NASA/ESTO using GLAS data and
will also reflect back on an earlier study of the LITE data.
[24]
The
design of an orbiting wind profiling lidar requires selection of dozens of
lidar, measurement scenario, and mission geometry parameters. Typical mission
designs do not include a thorough trade optimization of all of these
parameters. We report here the integration of recently published
parameterization of coherent lidar wind velocity estimation with an orbiting
coherent wind lidar computer simulation; and the use of these combined tools to
perform some preliminary parameter trades. We use the 2006 NASA Global Wind
Observing Sounder (GWOS) mission design as the departure point for the trades.
[25]
The
CALIPSO satellite is providing our first continuous observations of the global
three-dimensional distribution of aerosols and clouds. CALIPSO was launched in
April 2006 and has been acquiring lidar observations since June 2006. The
primary instrument on the CALIPSO satellite is CALIOP, a two-wavelength
polarization lidar designed for aerosol and cloud profiling. CALIOP has
sensitivity sufficient to detect clouds with optical depth less than 0.01 and
aerosol with scattering coefficients less than 1E-3 /km/sr. Ultimate
performance limits are still being assessed. This talk will discuss aspects of
CALIPSO and aerosol and cloud observations relevant to future Doppler wind
lidar missions
[26]
A
unique, multi-frequency, single-beam, laser absorption spectroscopy instrument
has been developed for space-based measurements of carbon dioxide (CO2) in the
troposphere. The system utilizes low-power narrow-band modulated-continuous
wave all fiber transmitter, with a high gain no excess noise APD detector and
narrow-band demodulation system to achieve high signal-to-noise ratios for
precision differential CO2 column optical depth measurements. A prototype
instrument and high-fidelity, physics-based performance model has been
constructed and validated through several years of ground, field and airborne
testing. The performance and advantages of this approach will be discussed
relative to other systems under consideration for space-based measurements of
CO2.
[27]
The
Global Carbon Cycle has been significantly perturbed by human activities in the
last two centuries. The current network is insufficient either to understand
the fundamental phenomena or to predict the future rate of increase of
atmospheric CO2 density and its impact on climate.
In this context, a 2 µm Heterodyne Differential Absorption Lidar (HDIAL) has
been developed and operated at IPSL/LMD to monitor CO2 mixing ratio in the
atmospheric boundary layer. In the present paper, we address the comparison of
the CO2 HDIAL measurements with in-situ sensors positioned along the path of
the laser beam: 1) a 2.064-µm Heterodyne Differential Absorption Lidar 2) a
field deployable Laser Diode Spectrometer (LDS) using new commercial diode
laser technology at 2.68 µm 3) LICOR NDIR gas analyzer 4) flasks. We present
the overall experimental set up i.e. DIAL and in situ measurements conducted at
the same location. Moreover, using several sensors of CO2 at different sites,
the campaign enables to quantify a gradient of CO2 in a near urban area and to
understand the impact of advection on the CO2 variability in the ABL.
[28]
The
National Institute of Information and Communications Technology (NICT) started
a new 5-year program to develop a coherent differential absorption lidar for
atmospheric CO2 measurement in April, 2006. Effects of atmospheric temperature
and laser wavelength uncertainties were investigated and candidate wavelengths
were selected. A high-energy pulsed single-frequency Tm:Ho:YLF laser was
developed and the laser operates at a pulse repetition frequency of 10 Hz and
emits an output energy of 100 mJ with pulse width of 120 ns (FWHM). The
receiver is based on a 10-cm-diameter off-axis telescope, 2-μm
waveguide coupler with a 50/50 split ratio, and balanced InGaAs photodiodes.
We present the coherent differential absorption lidar developing at the NICT.
[29]
A
new concept of DIAL (DIfferential Absorption Lidar) system for global CO2
monitoring is introduced. In this system, ON/OFF wavelength laser lights are
intensity modulated with CW modulation signal, and received lights of two
wavelengths from the ground are discriminated by modulation frequencies in
electrical signal domain. Fiber-based optical circuit using wavelength region
of 1.6 micron is suitable for the system configuration. After the explanation
of this configuration, feasibility study of this system, including the error
budget analysis in measurements, is introduced on the application to global CO2
monitoring.
[30]
The
method of buried landmine detection using low-frequency elastic waves in the
ground and a laser Doppler vibrometer (LDV) as a vibration sensor has shown
excellent performance in field tests. To reduce the time of detection, LDVs
with multiple probe beams and parallel signal processing have been developed.
A multi-beam LDV with linear array beam configuration can create a vibrational
image of the ground surface in a stop-and-stare or a continuously scanning
mode. A multi-beam LDV with probe beams configured into 2D-array is capable of
creating a vibrational image of the ground surface with a single shot
[31]
This
paper will review some recent laser sensing activities at FOI. Due to shift of
interest from our customer the coherent laser radar activities have been
limited so the main part of the paper will be devoted to direct detection laser
radars. Hopefully this overview will have some relevance for the CLR community.
The presented activities include 3 D imaging, terrain mapping, land mine
detection, aerosol lidar, bio detection, remote listening, high resolution
range profiling and laser development. We also have some limited activities in
retro communication, adaptive optics and beam steering. A recent review gives
examples of laser sensing at FOI and elsewhere of relevance for defense and
security applications
[32]
The
Super-resolution Sensor System (S3) program at Lockheed Martin Coherent
Technologies (LMCT) is an ambitious effort to exploit the maximum information a
laser-based sensor can obtain. We are exploring methods of incorporating
multi-function operation (3D imaging, vibrometry, polarimetry, aperture
synthesis, agile apertures, etc.) into a single device with waveforms matched
to the requirements of both hardware (e.g., optical amplifiers, modulators) and
the targets being imaged . The first successful demonstrations of this program
have produced high-resolution, 3D images at intermediate stand-off ranges,
heavy camouflage penetration, and adaptive techniques for draped multi-layer
obscurations.
[33]
Ladar
based vibrometry has been shown to be a powerful technique in enabling the
plant identification of machines. Vibration can be sensed reliably and provide
positive identification at ranges beyond the imaging limits of the aperture.
However, as the range of observation increases, the diffraction limited beam
size on the target increases as well, and may encompass multiple vibrational
modes on the target’s surface. As a result, vibration estimates formed from
large laser footprints illuminating multiple modes on a vibrating target will
experience a degradation. A model to predict this phenomenology is proposed
for pulse-pair vibrometry systems.
[34]
The
limitations of the turbulent atmospheric channel are examined by using the
simulation of beam propagation. The aim of this study is to consider how the
compensation of atmospheric turbulence wavefront phase distortion by using
modal methods improves the performance and reliability of free-space laser
systems based on the heterodyne detection scheme. In a process of tracking of
the beam wavefront and consequent correction of atmospherically-induced
aberrations, the aim of phase compensation would be to restore
diffraction-limited resolution. The modal correction of several modes of an
expansion of the total phase distortion in a set of basis functions may offer
the potential for overcoming some of the restrictions imposed by the atmosphere
in practical systems.
[35]
Expressions
for the bistatic gain of a coherent lidar are reviewed. We show that the
fundamental representation of the monostatic gain is in terms of the wander
corrected on-axis scintillation index and the wander corrected bistatic
gain.
[36]
:
In this paper, the performance of GAPD based ladar receivers is investigated
and a theory for the signal photon detection efficiency (SPDE) is developed as
a function of the dead-time; signal, noise and clutter flux; and the GAPD’s
photon detection efficiency or PDE. This efficiency theory is valid for
arbitrary (short to long) dead-times. With a zero dead-time, GAPDs behave
linearly and the efficiency theory converges to the PDE. For long dead-times,
compared to the acquisition gate time, the theory converges to previously
published works of Fouche and Williams. This SPDE theory is then applied to
develop other ladar metrics, e.g. SNR.
[37]
This
article presents our investigations into the physical and optical properties of
canopies and their individual scattering elements in order to develop an
improved foliage penetration model. We employed a Monte Carlo algorithm to
simulate the propagation of a pencil beam of photons through a canopy of
leaves. Simulations were made modeling the individual leaves as several
different bidirectional scattering distribution functions (BSDF). The spatial,
temporal, and angular point spread functions were measured for each BSDF and
compared such that an optimal canopy propagation model was created.
[38]
Coherent
detection of optical signals offers many benefits for
fiber optic communications, but has been regarded as prohibitively complex
to implement. Recently a mode of coherent detection has been proposed which
overcomes these issues using real time digital signal processing.
Experimental results are presented showing how the information is recovered when
the signal and local oscillator are combined in a phase diverse hybrid,
and good receiver sensitivity is achieved. Fiber propagation
impairments can be compensated within the digital processor, and compensation of
chromatic dispersion and polarisation mode dispersion is demonstrated. Some
of the future possibilities for coherent dection are described.
[39]
The
Laser Interferometer Gravitational-Wave Observatory (LIGO), consisting of three interferometers at the two LIGO observatory
sites (Livingston, LA and Hanford, WA), is operational and the LIGO
Scientific Collaboration is embarked on a several-year period of searching
for gravitational wave emissions from astrophysical sources. The threshold for measuring gravitational waves as length changes between two
test masses is extremely low, requiring extremely high accuracy in the sensitivity to length changes. Each LIGO detector is a
power-recycled Michelson Interferometer with Fabry-Perot cavities in the 4 km long arms. All optical elements, and the laser beam between them, operate in UHV. In this talk, I will
discuss the operation of the LIGO interferometers, and the techniques that were used to reach a sensitivity of 10^-18 m/sqrt(Hz) for 100 Hz signals.
Supported by the NSF grant PHY-0555453.
[40]
Coherent
laser communication terminals based on homodyne BPSK (binary phase shift
keying) combine highest sensitivity for both, communication and tracking, with
immunity against sunlight. We report on a new generation of coherent terminals
for a LEO-GEO data relay system to transmit data from TanDEM-X, a German LEO
earth observation satellite to a European GEO satellite with a Ka-band
downlink. The system will be extended to optical GEO-to-ground links using
adaptive optics on ground. All optical inter-satellite links are duplex links
with a foreseen data rate of 2.8 Gbps.
[41]
Flight
demonstrations have proven the feasibility of synthetic aperture LADAR (SAL)
imaging and have produced outstanding imagery of vehicles and engineering test
targets. These tests were conducted under the Synthetic Aperture LADAR for
Tactical Imaging (SALTI) program. SALTI is a Defense Advanced Research Project
Agency program executed with the Air Force Research Laboratory, Sensors
Directorate which has demonstrated practical SAL architectures. The
atmospheric and target phenomenologies were investigated for both short wave
infrared (SWIR) and long wave infrared (LWIR) systems and the relevant are
compared with some basic SAR parameters. An introduction to the SAL systems is
presented, representative simulated images are shown and turbulence driven
performance regimes are discussed. Finally, test objectives of a third series
of tests and future plans are presented.
[42]
With
a multi-aperture imaging system, one creates a large imaging aperture by
combining the light from a series of distributed telescopes. In doing this, one
can construct a fine-resolution imaging system with reduced volume. We present
work on multi-aperture, active imaging systems that use coherent detection and
digital image formation. In such a system, the image formation process
incorporates digital correction of optical and atmospheric phase errors. Here
we discuss the principles underlying this method and present results from
laboratory experiments and field experiments performed over a 0.5 km outdoor
test range. In addition we discuss 3D imaging capability of the method
[43]
A
primary goal of sparse aperture imaging is to enhance resolution while
minimizing the total light collection area, the latter being desirable, in
part, because of the cost of large, monolithic apertures. We construct arrays
by locating multiple, identical circular sub-apertures and evaluate array
performance based on PSF and MTF metrics. We select an optimal array
constructed on a compact nonredundant point array first described by Golay. We
report experimental results of imaging a resolution target from by masking a
large lens with the Golay array noting the loss of image contrast inherent to
sparse arrays.
[44]
Recently
a great deal of work has focused on the use of nonclassical states of light for
performing measurements with precision beyond that attainable with the usual
coherent laser light. Laser radar poses special challenges for the use of
nonclassical states due to the large losses involved in typical laser radar
applications. We examine the possibility of employing squeezed states and
maximally-entangled (“NOON”) states in laser radar, and find that the presence
of loss severely limits their potential utility
[45]
This
talk will present the first experimental demonstration of coherent detection
using an array of photon-counting detectors. These measurements use an array
of Geiger-mode avalanche photodiodes with integrated CMOS timing circuitry, and
show the potential for shot-noise-limited detection in the single-return-photon
regime with comparable local oscillator power. The high-bandwidth timing
circuitry and potential to fabricate large arrays enable range-resolved Doppler
and angularly-resolved Doppler laser radar measurements. Laboratory results
agree well with theory and computer simulations.
[46]
Passively
mode-locked fiber lasers produce a broad, yet phase-coherent output spectrum.
In the frequency domain, this output forms a frequency comb, where each comb
line corresponds to an individual laser mode. We will discuss using a
frequency comb in a coherent LIDAR system for high resolution range or Doppler
measurements. In order to effectively use the broad spectrum, we spectrally
resolve the signal into discrete bands, apply any necessary phase compensation,
and then Fourier-process the data to produce a range image or Doppler
signature. We will discuss both our initial experiments and future efforts
using two phase-coherent frequency combs.
[47]
Our
terahertz-based vibrometer measures at a standoff, vibrations behind optically
opaque barriers, such as cardboard, clothing and plastic. Its Michelson-based
design gives sub-micron sensitivities, which are limited by the detector. We
use commercially available, room temperature components. Measured spectral
response compares favorably with optical vibrometry without barriers.
[48]
The
measurement of various atmospheric parameters is of great importance to
understand physics, chemistry and dynamics. The Lidar has proved to be an
important tool for atmospheric probing. Various types of Lidar systems have
been used for atmospheric monitoring since the invention of laser by Maiman in
early 1960s to measure various atmospheric parameters such as aerosols, minor
constituents, wind, temperature etc. Keeping above in view we at National
Physical Laboratory, New Delhi have designed and developed a high resolution
Laser Heterodyne system with 1 GHz acousto-optical spectrometer as backend for
vertical profiles of various trace species including ozone profiles at Maitri,
Antarctica during normal as well as ozone hole conditions, Differential
Absorption LIDAR (DIAL) for monitoring of surface ozone, water vapour,
ammonia, ethylene etc and Micro Pulse lidar for vertical profiles of aerosol
and their characterization using depolarization ratio measurements.!
Also appropriate inversion
technique has been developed for retrieval of ozone profiles. In the present
communications the salient features of the systems developed at NPL and
results obtained will be discussed in detail.
[49]
We
describe and demonstrate a sensitive room-temperature detection of terahertz
radiation by nonlinearly upconverting terahertz to the optical near-infrared
regime, relying on telecomm components. Terahertz radiation at 700 GHz is
mixed with pump light at 1550 nm in a bulk GaAs crystal to generate an idler
wave at 1555.6 nm which is separated and detected using a commercial PIN diode.
The THz detector operates at room temperature and has terahertz-to-optical
photon conversion efficiency of 0.001%.
[50]
The
2-micron thulium and holmium-based lasers being considered as the transmitter
source for space-based coherent Doppler lidar require high power laser diode
pump arrays operating in long pulse regime of about 1 msec. Operating laser
diode arrays over such long pulse duration drastically impact their useful
lifetime due to the excessive localized heating and substantial pulse-to-pulse
thermal cycling of their active regions. This paper describes the long pulse
mode performance of laser diode arrays and their critical thermal
characteristics. A viable approach is then offered that allows for determining
the optimum operational parameters leading to the maximum attainable lifetime
[51]
Three-dimensional
imaging ladar sensors can be used for terrain mapping missions. Photon counting
receiver arrays provide the systems engineer with the ability to make important
system trades of range capability, receiver aperture, laser size and ladar FOV.
MIT/LL has pioneered Geiger mode APD array receivers for ladar systems that
provide photon counting sensitivity in a 32x32 array with good range resolution
capabilities.
Boeing SVS, Boeing Spectrolab and MIT/LL have entered into a tech transfer
relationship to bring MIT/LL Geiger Mode APD arrays out to industry. The tech
transfer project for the 32x32 InGaAsP arrays can be broken down into 5
components, each being handled and funded by different parties. 1. Material
growth; 2. Material Characterization; 3. Detector array fabrication; 4.
Packaging; 5. Electronics and Real Time Processor. This presentation will
provide progress and performance details for all 5 areas and give data examples
from a terrain mapping field collection.
[52]
The
use of lidars in ground, airborne, and space-based missions can provide earth
and planetary science measurements that were previously unavailable. Our
approach to the laser transmitters needed for such systems focuses on
developing environmentally hardened prototypes whose designs can be validated
with extensive testing. We applied this approach to the laser transmitter for
the CALIPSO aerosol lidar mission by designing and testing the Risk Reduction
Laser. We are in the process of a similar development effort for the injection
seeded single frequency lasers that will be needed for the next generation of
airborne and space-based lidar systems
[53]
Photoacoustic
technique is introduced as a convenient and accurate method for the control of
laser spectral shift. A non resonant photoacoustic cell (PAC) is investigated
to monitor a pulsed laser spectral shift on a CO2 absorption line in the 2-µm
domain. A minimum ~ 1 % of accuracy on CO2 Heterodyne Differential Absorption
Lidar (HDIAL) measurement is estimated when the laser is tuned to the centre of
the absorption line.
[54]
Tesat
Spacecom has build and tested the flight models of the Reference Laser Head
(RLH) for the ESA AEOLUS mission, a space borne UV LIDAR system. The RLH
provides frequency stable (4 Hz / sec absolute long time frequency drift) and
tunable (8.333 GHz in 8.333 MHz steps) single frequency light at 1064n. It is
used as seeder input for the pulsed laser system. The design and flight model
performance results for the RLH are shown.
[55]
subtitle:
Eyesafe 1.6 μm Er:YAG transmitters for coherent laser radar
[56]
Reconstruction
of wind profile based on the turbulent spatio-temporal statistics of reflected
optical wave focused by the receiving telescope is considered. Both the
expression for the spatial temporal correlation function and spectrum and the
algorithm of wind profiling based on the spatio-temporal spectrum of weak
intensity fluctuations of a wave scattered off diffuse target are presented.
Computer simulations performed under conditions of weak optical turbulence show
wind profiles reconstruction by the developed algorithm
[57]
Numerous
treatments in the literature over the years have concluded that heterodyne
efficiency, and thus heterodyne signals from diffuse targets, decrease as
detection apertures increase, based on the mistaken assumption that signals
decrease as phase and intensity correlations decrease. Random walk models for
laser speckle phenomena suggest that signal strength (carrier-to-noise ratio)
always increases (on the average) with aperture, however care must be taken to
match the divergence and intensity of the local oscillator to optimally achieve
the increased CNR. Theory and examples will be given to justify the
conclusions.
[58]
Low-level
turbulence is an aviation hazard. This paper discusses the use of glide-path
scan of the LIDAR at the Hong Kong International Airport to calculate
turbulence intensity. Structure function approach based on the radial velocity
data of the LIDAR is adopted. The turbulence intensity so determined is
compared with pilot reports to illustrate the potential application of the
method for turbulence alerting.
[59]
Looking
ahead of the aircraft in search of vertical motions has usually been done with
conical scans of small cone angles. Recent experiments have been performed
using raster scans ahead of the aircraft to collect Line-of-Sight velocity data
from which the nearly orthogonal vertical motion can be inferred.
The raster scan approach was tested in cloud free conditions over Monterey Bay
(CA), the Salinas Valley and the nearby mountain ranges. The experiments
revealed useful relationships between aerosol returns and LOS velocity
convergence.
This presentation will present results of those flights and discuss
implications to aircraft flight control and turbulence avoidance.
[60]
Multipixel
coherent receivers are not yet commonplace. However, these types of receivers
are gaining popularity and it is important to understand their measurement
limits. In particular, the angle estimates (from a centroiding technique)
produced by a coherent array are intimately tied to the LO pattern on the
receiver. This work examines the angle estimation error from one example
arrangement. This theory is then shown to compare favorably to Monte Carlo
simulation results.
[61]
Lidar
measurement of oceanic temperature and sound speed by measuring the spectral
shift of the backscattered Brillouin doublet has been proposed in previous
studies. Technical limitations on both transmitter and receiver have until now
prevented experimental demonstration at 1 m/sec accuracy. Receiver
requirements are met by utilizing an edge technique based on absorption lines
of an iodine isotope. With edge filtering, small changes in frequency shift of
the Brillouin doublet produce significant change in the transmission through
the iodine vapor. The resulting filter transmission signal has a one-to-one
correspondence with water temperature (hence sound speed). Our laboratory
measurements demonstrate this.
[62]
Coherent
imaging provides a means to do multi-aperture imaging without the need for
complex sensors, actuators, and control systems that a passive multi-aperture
imaging system requires. However, this mechanical complexity is traded for the
processing complexity involved in producing the synthetic image. In this paper,
the development of a multi-aperture coherent imaging testbed which aims to
implement high speed processing is described, and some preliminary tests in
both multi-aperture and three-dimensional imaging are documented.
[63]
We
generally accept the experimentally observed criteria for heterodyne detections
that the two waves that are mixed must (i) be collinear, (ii) have matched wave
fronts and (iii) cannot be orthogonally polarized. We find that there are a
number of unresolved paradoxes in classical and quantum optics regarding the
definitions and understanding of the “interference” and “coherence” properties
of light, which are attributed as essentially due to inherent properties of the
EM waves. The purpose of this paper is to find deeper physical understanding
of the heterodyne detection processes that could lead to better laser radar
system design.
[64]
Averaging
is often used in processing coherent lidar data to reduce noise fluctuations
and improve the ability to detect the presence of a target. There are many
choices of averaging techniques, and this work examines two types of averaging
filters. The first is an FIR filter that has often been used in the past and
is well understood. The second is an IIR filter that is also common in
practice, but has not been carefully analyzed. This work compares the
detection performance between these two types of filters and points out the
advantages and disadvantages of each.
[65]
We
explain Level-2B/Level-2C products from the ADM-Aeolus mission. These products
aim at providing meteorologically representative wind profiles, meeting neos of
user communities in operational numerical weather prediction and more general
atmospheric science. Whereas Level-2B profiles report single wind components
(along the horizontal line-of-sight), Level-2C profiles report wind vectors
(two horizontal components).
We cover a) the theoretical basis of the retrieval algorithms, and b) details
of how to obtain the Level-2B processor portable source code - designed for use
as either 1) a standalone executable in a general scientific environment, or 2)
a callable subroutine integrated within a data assimilation system.
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