13th International Laser Ranging
Workshop
"Toward Millimeter Accuracy"
Submitted
Abstracts
Detectors and Optical Chain Components (G. Kirchner and L. Grunwaldt)
Title |
Primary Author |
New Detection Package at Graz |
Georg Kirchner |
Austrian Academy of Sciences
Observatory Lustbuehel
Lustbuehelstrasse 46
A-8042 Graz
AUSTRIA
Voice: +43-316-873-4651
Fax: +43-316-873-4641
Email: kirchner@flubpc04.tu-graz.ac.at
Franz Koidl
Austrian Academy of Sciences
Observatory Lustbuehel
Lustbuehelstrasse 46
A-8042 Graz
AUSTRIA
At present, SLR Graz is using a simple, straightforward detection
package: After the main receiving telescope, the 14 mm beam passes
a 0.3 nm interference filter, and is focused on the C-SPAD surface.
While this setup is simple, stable and reliable, the 0.3 nm filter
usually only allows a maximum of 30% to 40% transmission; it is
also difficult to operate it in MultiColor schemes.
To improve the total transmission of the optical receiver channel,
we are building now a new detection package, which uses dispersion
for wavelength filtering as well as for wavelength separation
for MultiColor Operation. Because the effective filter bandwidth
will be less than 0.15 nm, and the overall transmission of the
receiver package should be more than 70% due to omitting any interference
filter, the calculated improvement in signal to noise ratio should
be a factor of 4. In addition, the dispersion scheme allows for
efficient wavelength separation, again with minimized optical
losses.
Oral paper; received August 9, 2002
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The advantages of Avalanche Photodiode (APD) arrays
in laser ranging applications |
Jana Strasburg |
University of Washington
Box 351560
Seattle, WA 98195
USA
Voice: 206-543-8989
Fax: 206-685-0635
Email: jdstras@u.washington.edu
T. Murphy, C. Stubbs, E. Adelberger
University of Washington
Box 351560
Seattle, WA 98195
USA
The Apache Point Observatory Lunar Laser-ranging Operation (APOLLO)
is a new lunar ranging campaign aimed at achieving millimeter
precision. At the heart of APOLLO is an integrated array of avalanche
photodiodes developed at MIT's Lincoln Laboratories. These devices
are capable of detecting the arrival of a single photon with high
temporal precision (< 50 ps), at detection efficiencies as
high as 50%. The integrated array format allows one to create
a range profile with each laser shot by detecting multiple return
photons, thereby eliminating the strong-signal biasing encountered
with a single detector. The array format also preserves spatial
information, facilitating target acquisition and tracking. We
are currently using a 4 x 4 array, but the timing system can easily
be multiplexed to handle arrays of 10 x 10 elements or larger.
Lincoln Labs is presently testing 32 x 32 devices.
Oral paper; received August 20, 2002
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Characterization of a Microchannel Plate Photomultiplier
Tube with a High Sensitivity GaAs Photocathode |
Paul H ink |
1000 New Holland Avenue
Lancaster, PA 17601
USA
Voice: (717) 295-6373
Fax: (717) 295-6096
Email: martinj@burle.com
Charles Tomasetti, Joesph Wright, John Martin
1000 New Holland Avenue
Lancaster, PA 17601
USA
Presented by: John Martin
The characteristics of an 18mm photomultiplier tube (PMT) having
a high sensitivity GaAs photocathode have been studied. This PMT,
the BURLE 85104, uses a dual microchannel plate (MCP) electron
multiplier. We report measurements that include standard DC response,
single electron sensitivity and resolution, time response, pulse
and count rate linearity, and dark counts as a function of temperature.
Data is also presented for a gated version of the PMT that has
a high-speed anode. The properties of these MCP-PMTs make them
well suited for applications such as LIDAR, fluorescence microscopy
and chemiluminescence.
Oral paper; received August 21, 2002
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Time walk compensation of a SPAD with linear photo
detection |
Etienne Samain |
OCA
2130 Route de l'Observatoire
06460 Caussols
FRANCE
Voice: 33 4 93 40 54 29
Fax: 33 4 93 40 54 33
Email: etienne.samain@obs-azur.fr
The photo detection with a photo diode in the Geiger mode appears
promising because of the time stability, the sensitivity, and
the simplicity of the device. The transit time between the pulse
arrival and the moment when the signal reaches a given detection
threshold depends on the photon number in the light pulse. A precise
knowledge of this photon number permits to eliminate this time
walk if a correction table is known. A device using an auxiliary
linear light sensor to measure this photon number coupled with
a photo-diode in the Geiger mode for the timing purpose is presented
here. This device is designed for both the space and ground segment
of the T2L2 (Time Transfer by Laser Link) experiment and could
be used in the frame of the satellite laser ranging activities.
Oral paper; received August 23, 2002
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SPAD Detector Package for Space Born Applications |
Ivan Prochazka |
Czech Technical University in Prague
Brehova 7
115 19 Prague 1
CZECH REPUBLIC
Voice: +420 723 920786
Fax: +420 2 57210282
Email: prochazka@mbox.cesnet.cz
The SPAD detector package for the space born applications is
under development for several space missions (T2L2 experiments,
transponder, altimeter). The detector is based on the SPAD chips
with and active area with 25 um diameter and a newly designed
active quenching and gating circuit. The ultra short circuit dead
time permits to operate the SPAD in both gated and ungated modes
with dark count rates below 10 kHz and timing resolution better
than 100 psec. The first results will be presented.
Oral paper; received August 28, 2002
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Testing of MCP PMTS: Use of Fiber Optic Coupled
Gbps Laser Drivers to Create Ersatz Laser Return Pulses |
Thomas Cuff |
Honeywell-TSI
7515 Mission Drive
Lanham, MD 20706
USA
Voice: 301.805.3946
Fax: 301.805.3974
Email: thomas.cuff@honeywell-tsi.com
Richard Chabot
Honeywell-TSI
7515 Mission Drive
Lanham, MD 20706
USA
From an operational point of view, it is important to be able
to test the MCP (Micro Channel Plate) PMT (PhotoMultiplier Tube)
front end of LIDAR transceivers used in SLR (Satellite Laser Ranging)
work. In the day-to-day operation of SLR systems, one needs to
have an independent method of ascertaining that the receiver half
of the LIDAR transceiver is functioning properly. In addition,
the sensitivity and stability of the MCP PMT front end of the
LIDAR transceiver also needs to be periodically checked against
a standardized source to prevent long and short term errors from
insinuating themselves into the production data stream. The creation
of ersatz laser return pulses is also useful when developing new
LIDAR systems such as NASAs micro-laser altimeter and SLR2k
robotic observatory. This paper describes a number of ways of
constructing a laser return pulse generator from COTS (Commercial
Off The Shelf) parts. In particular, we detail the use of currently
available single chip laser drivers normally employed in
fiber optic LAN (Local Area Network) and WAN (Wide Area Network)
telecommunication systems as the heart; of
the generator. Fiber optics is used to plumb; the
ersatz laser return pulses together with the optical noise baseline
to the output connector of the generator. The use of fiber optics
allows one to conveniently fold the optic path within the generator
without utilizing mirrors or prisms needed in a free space design
and so results in a flatter volume for the generator and obviates
the need for enclosing the generator in a light tight box. Since
the specifying and ordering of single chip laser drivers and fiber
optic components involve considerable amounts of jargon this aspect
will also be covered.
Oral paper; received September 06, 2002
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