Title: Theoretical Centreofmass Corrections for LAGEOS, ETALON and AJISAI
1Theoretical Centre-of-mass Corrections for
LAGEOS, ETALON and AJISAI
See Otsubo and Appleby, JGR, 108, B4, 2201, Apr
2003.
- Toshimichi OTSUBO
- Communications Research Laboratory, Kashima,
Japan - Graham M APPLEBY
- Natural Environment Research Council, Monks Wood,
UK
Laser Workshop 2003, Koetzting, 28-31 Oct 2003.
2Satellite signature effect
- Multiple reflectors contributing to the satellite
response. - System-dependent detection timing.
- Single photon
- C-SPAD
- MCP-PMT
- Key error factor to achieve accurate GM and TRF
scale.
3ETALON(12) USSR 1989 Altitude 19000 km Diameter
1.294 m 2134 CCRs
AJISAI Japan 1986 Altitude 1500 km Diameter 2.15
m 1436 CCRs
LAGEOS(12) USItaly 1976, 92 Altitude 5900
km Diameter 0.60 m 426 CCRs
4Response from single reflector
- 3 factors to be considered.
- Effective reflection area (a)
- Reflectance (e)
- Diffraction
- How to compute the intensity.
- ?ae diffraction neglected.
- ?a2e simple diffraction model.
- Neubert, 1994 Otsubo, 1999
- ?ane this study.
5- ? Effective reflection area
Reflectance ?
6Centre-of-mass correction
Extracted from Otsubo and Appleby, JGR, 108, B4,
2201, Apr 2003.
0.25
0.24 (m)
251 Standard
257.6 r - nL
247
249
250
252
(n2.0)
Single Photon
245 Hx
245 3-sigma
242 w/o clipping
250 2-sigma
247 2.5-sigma
C-SPAD
245 Ideal S.P. (lt0.1 p.e.)
249 1 p.e.
257 100 p.e.
256 10 p.e.
PMT (LEHM)
248 300 ps
244 1ns
256 1 ps
242 3ns FWHM
252 100 ps
7Centre-of-mass correction
Extracted from Otsubo and Appleby, JGR, 108, B4,
2201, Apr 2003.
1.00
0.95 (m)
1010 Standard
1028 r - nL
977
(n2.0)
987
993
1002
Single Photon
985 Hx
976 3-sigma
962 w/o clip
985 2.5-sigma
997 2-sigma
C-SPAD
1023 100 p.e.
1020 10 p.e.
977 Ideal S.P. (lt0.1 p.e.)
990 1 p.e.
PMT (LEHM)
1009 300 ps
976 3 ns FWHM
1022 1 ps
1017 100 ps
993 1 ns
8Centre-of-mass correction
Extracted from Otsubo and Appleby, JGR, 108, B4,
2201, Apr 2003.
0.60
0.55 (m)
576 Standard
613 r - nL
570
575
582
593
(n2.0)
Single Photon
565 Hx
552 w/o clip
556 3-sigma
580 2-sigma
564 2.5-sigma
C-SPAD
558 Ideal S.P. (lt0.1 p.e.)
613 100 p.e.
573 1 p.e.
608 10 p.e.
PMT (LEHM)
607 100 ps
598 300 ps
612 1 ps
562 3 ns FWHM
578 1 ns
9Discussions (personal opinions) for mm ranging
- Avoid the intensity-dependent bias ON-SITE!
- Likely to become the elevation-angle-dependent
bias, which can significantly degrade the station
height determination. - C-SPAD does NOT compensate the satellite returns.
1 cm for LAGEOS, 4-5 cm for AJISAI and ETALON. - MCPCFD seems ok at 1-cm level, but not at 1-mm
level. - Try the on-site shot-by-shot experiment.
- kHz laser? Go for STRICT single photon!
10Range residuals vs Intensity (Otsubo and
Genba, DC Workshop, 2002)
11Range residuals vs Intensity (Otsubo and
Genba, DC Workshop, 2002)
12Range residuals vs Intensity (Otsubo and
Genba, DC Workshop, 2002)
13Discussions (personal opinions) for mm analysis
- Better adjust the range bias for a while.
- 1-mm accuracy is still a challenge.
- Impossible to model the CoM correction for
multi-photon (esp. MCPCFD) systems at 1-mm
accuracy. - Many other systematic error sources.
- Accept a constant offset bias. Too risky to fix
it to 0 mm. - Tight constraints can be applied if necessary.
- A different story when all stations do the single
photon.
14Summary
- Stations,
- Eliminate any systematic range errors.
- Analysts,
- Not assume zero range bias.
- English speakers,
- Is the word bias appropriate? Probably
negative impression to non-SLR people.
15Satellite Signature Effect in GLONASS SLR Data
- Toshimichi OTSUBO
- Communications Research Laboratory, Kashima,
Japan - Graham M APPLEBY
- Philip GIBBS
- Natural Environment Research Council, Monks Wood,
UK
Laser Workshop 2003, Koetzting, 28-31 Oct 2003.
16GLONASS CCR Array
New type (except GLO-88) - 132 CCRs. - Since
GLO-84.
Old type - 396 CCRs. - Until GLO-80.
17(No Transcript)
18(No Transcript)
19(No Transcript)
20old
Effective array size estimation - for 2001. -
estimated by concerto ver 3. - bias
elevation dependent average (eff array size)
x 0.15 .
old
NEW
21NEW
Effective array size estimation - for 2002.
NEW
NEW
22Summary
- GLONASS CCR Design
- Large flat array is probably not the best idea.
It causes the elevation-dependent range error.
2 cm on average. - New CCR array at least halved the signature
effect. lt 1 cm on ave. - Return energy vs signature effect
- Difficult in observing new GLONASSes esp in
daytime? - What is the best array pattern for such high
orbiters? - How about in the GALILEO project?
-