Progress on Laser Time Transfer Project Progress on Laser Time Transfer Project Yang Fumin Yang Fumin (1) Huang Peicheng (1) Chen Wanzhen (1) Zhang Zhongping (1) Wang Yuanming (1) Chen Juping (1) Guo Fang (1) Zou Guangnan (2) Liao Ying (2) Ivan Prochazka (3) Karel Hamal (3) (1) Shanghai Observatory, Chinese Academy of Science, Shanghai, China (2) China Academy of Space Technology, Beijing, China (3) Czech Technical University in Prague, Czech Republic
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Progress on Laser Time Transfer ProjectProgress on Laser Time Transfer Project
Yang FuminYang Fumin(1) Huang Peicheng(1) Chen Wanzhen(1)
Zhang Zhongping(1) Wang Yuanming(1) Chen Juping(1) Guo Fang(1)
Zou Guangnan(2) Liao Ying(2) Ivan Prochazka(3) Karel Hamal(3)
(1) Shanghai Observatory, Chinese Academy of Science, Shanghai, China
(2) China Academy of Space Technology, Beijing, China
(3) Czech Technical University in Prague, Czech Republic
GoalsGoals
•• Evaluation of performance of space clocksEvaluation of performance of space clocks
-- now for now for rubidiumsrubidiums
-- in future for hydrogen masersin future for hydrogen masers
•• Verification of the relativityVerification of the relativity
2τ
GT T∆
ST
2τ
Ground Time
Satellite Time
Transmitted
Laser Pulse
Clock
SecondReceived
Laser Pulse
Returned
Laser Pulse
Clock
Second
2G S
T T Tτ
∆ = − −
Principle of Laser Time Transfer (LTT)Principle of Laser Time Transfer (LTT)
Diagram of LTT between Space and Ground
The LRA for LTT Experiment
• The orbit of the satellite for the LTT
experiment will be about 20000KM
• The LRA is a planar panel
• 42 retros with aperture of 33mm
• Total reflective area is 360cm2
• Total mass is 2.5 Kg
Block Diagram of LTT ModuleBlock Diagram of LTT Module
Specifications of the DetectorSpecifications of the Detector
� configuration dual photon counting detector
based on Silicon K14 SPAD
� active area circular 25 um diameter
� timing resolution < 100 psec
� operating temp. -30 … +60oC
no cooling, no stabilisation
� power consumption < 400 mW
� optical damage th. full Solar flux 100 nm BW, > 8 hr
� lifetime in space > 5 years
LTT DetectorLTT Detector
Dual SPAD detector, 300g, <1W, 105××××70××××50mm
Field of View: 30°°°°, 10nm bandwidth filter
Estimate of the Received PhotonsEstimate of the Received Photons
by the Onboard Detectorby the Onboard Detector
The number of photons (NThe number of photons (NPP) received by the onboard detector ) received by the onboard detector
can be estimated by:can be estimated by:
2 2
4P t r
P
t
E S A K K TN
R
α
π θ
⋅ ⋅ ⋅ ⋅ ⋅ ⋅ ⋅=
⋅ ⋅
αααα: Attenuation factor, 0.5
θθθθt: Divergency of laser beam from telescope, 10 arcsec
R: Range of satellite, for MEO orbit at elevation 30°°°°,
22600Km
T: Atmospheric transmission (one way), 0.55
Kr: Eff. of receiving optics, 0.60
Kt: Eff. of transmitting optics, 0.60
AP: 40µµµµm SPAD without any lenses, diameter of active area,
0.025mm
S: Number of photons per joule (532nm), 2.7××××1018
WhereE: Laser pulse energy, 50mJ(532nm)
We have,We have,
Np=7.0 (Photons)
It can be detected by the 40 It can be detected by the 40 µµµµµµµµm SPAD detector.m SPAD detector.
Principle of the LTT TimerPrinciple of the LTT Timer
Principle of the TDCPrinciple of the TDC
( Time to Digit Converter( Time to Digit Converter——from Germany )from Germany )
Specification of the Timer
� Resolution of timing 10ps
� Precision of timing 100ps
� Mass (dual-timer) 4.3Kg
� Power consumption 17W
� Size 240××××100××××167mm
Top View of the LTT TimerTop View of the LTT Timer
Results of the Ground TestsResults of the Ground Tests
196.435.709±±±±
0.092Mean
96221.635.488249597.5249633.06374.8
90199.835.619249640.7249676.36187.9
103224.135.687249702.0249737.75923.8
96231.235.731249745.7249781.45736.5
5673.135.792249800.5249836.35498.9
84212.935.751249911.1249946.85022.8
148266.735.748250012.8250048.64588.9
136165.335.742250092.6250128.34246.1
139190.635.783250160.5250196.33953.8
104178.435.754250264.7250300.43508.7
Number of
Measurement
RMS((((ps))))(1)---- (2)((((ns))))(2)
Clock Difference
by Counter ((((ns))))(1)
Clock Difference
by Laser((((ns))))Epoch((((s))))
Results of LTT with two Results of LTT with two RbRb ClocksClocks
Red line:Red line: from LTT, slope:from LTT, slope: ((--2.32792.3279±±±±±±±±0.0012) 0.0012) ××××××××1010--1010
Black line: Black line: from SR620, slope:from SR620, slope: ((--2.32852.3285±±±±±±±±0.0011) 0.0011) ××××××××1010--1010
Dif
feren
ce o
f C
lock
s (n
s)D
iffe
ren
ce o
f C
lock
s (n
s)
Time (sec)Time (sec)
Uncertainty of measurement for the relative frequency Differences by laser link for
two rubidium standards is: 1.2××××10-13
2 sets of LTT Results with 2 2 sets of LTT Results with 2 RbRb ClocksClocks
Uncertainty for measuring relative frequency differenceUncertainty for measuring relative frequency differenceabout 4about 4××××××××1010--1313 in 200 seconds.in 200 seconds.
435580
435600
435620
435640
435660
435680
23450 23500 23550 23600 23650 23700 Time(s)
slope: (3.6601土0.0038)*E-10
Clock difference(ns)437160
437180
437200
437220
437240
437260
27800 27850 27900 27950 28000 28050
Time(s) slope: (3.6625土0.0045)*E-10
Clock difference(ns)
Uncertainty for measuring relative frequency difference Uncertainty for measuring relative frequency difference
about 5about 5××××××××1010--1414 in 1000 secondsin 1000 seconds