clock comparisons: present and future approaches
TRANSCRIPT
Clock Comparisons: Present and Future Approaches
IntroductionI. Dissemination of Legal TimeII. Comparisons of Time ScalesIII. Comparisons of Primary Clocks
MicrowaveTime & Frequency ComparisonsGPS P3 GPS carrierTWSTFT
Future PossibilitiesImproved Microwave Links (Reports by Ch. Salomon, W. Schäfer)Time Transfer by Laser Link (T2L2)Frequency Transfer by Fibre Links
Fritz Riehle(A. Bauch, D. Piester, H. Schnatz, ...)Physikalisch-TechnischeBundesanstalt, Braunschweig Germany
Workshop on an Optical Clock Mission in ESA’s Cosmic Vision Program, Düsseldorf, March 8, 2007
I. Time for the Public (PTB)Telephone time service
(1000 calls per day)
Internet Service(> 30 million accesses per day
DCF77(> 20 million receivers in Europe)
1 ms everywhere in Germany,Synchronization of phone networks, power plants, aviation security, ...
According to a market report (2001): The VAT from DCF77 related productsexceeds the provisions for DCF 77 by 14 times
II. Comparison of National Time Scales
51384 51744 52104 52464 52824 53184
-100
-80
-60
-40
-20
0
20
40
60
80
100
PTB NIST OP IEN NPL USNO
[UTC
–U
TC(k
) ] /
ns
MJDUTC – UTC(k) July 1999 – July 2004
III. Comparisons of Primary Clocks
FOUNTAIN
uB ≤ 10-15
H-Maser
FOUNTAIN
uB ≤ 10-15
H-Maser
TWSTFT
GPS CP
GPS TAI P3
?
Campaign: MJD 53304 – 53324 ( .. 53330) (Oct. / Nov. 2004)
R. Dach (AIUB), G. Petit (BIPM), L. Lorini (IMGC), P. Whibberley, R.Hlavac (NPL), T. Parker (NIST), J. Achkar, P. Uhrich (OP), A. Bauch (PTB): Time and Frequency Comparisons between fourEuropean Timing Institutes and NIST Using Multiple Techniques: EFTF 2005, Besancon
Time Transfer Technique I: GPS TAI P3
Input data: dual-frequency P1 and P2 code observables from „geodetic“ GPS receivers
Processing:Linear combination to provide ionosphere-free P3 observableTransfer to CGGTTS format:
track length 16 minutes, non-continuous observationCorrections applied: precise satellite orbits, satellite clocks provided by IGS
station displacements (solid Earth tides)
Evaluation of links in common view (CV) mode, 16 minute-averages formedby weighting individual CV data according to satellite elevation.
Reference: Defraigne and Petit, Metrologia 40 (2003), p. 184
Time Transfer Technique II: Carrier Phase
• Contributions of the Centre for Orbit Determination in Europe to IGS, Bernese GPS Software, Version 5.1
• new algorithm for GPS CP:
• ambiguities are connected at the day boundaries, consequently no discontinuities anymore
• only carrier phase measurements analyzed (no code data used)• applied fot the first time during this campaign
• GPS CP provides:• consistent receiver clock estimates for each epoch (once every 30 s)• no assumptions for the clocks from epoch to epoch
Use of estimates once every hour for GPS CP comparison betweenhydrogen masers
Time Transfer Technique III: TWSTFT
TWSTFT sessions co-ordinated by the CCTF Working Group on TWSTFT
TWSTFT using PRN-modulated signals (Mitrex or Satre modems) in Ku-band
Satellite transponder on IS-903 provided free of charge by Intelsat
Links between pairs of stations lasting 120 s once every two hours (12 sessions per day)
Availability: some links 3 to 5 missing points out of 320 (25 days)some links up to 20 points missing
Evaluation and report of data according to ITU-R Recommendation ITU-R TF.1153-1“The operational use of two-way satellite time and frequency transfer employingPN time codes”, ITU, Geneva, last update 2003.
Comparison of techniques (Link: NPL – OP)
Residuals after removing quadratic trend individually
TAI P3
GPS CP
TWSTFT
Comparison of techniques (Link: NPL – OP)
Instability of the relative frequency difference H-Maser(OP) – UTC(NPL)
GPS TAI P3
GPS CP
TW
GPS CP - TW
Summary (Instability achievable in 1 day)
TWSTFT: modσy < 1x10-15 collecting 12 points per day
GPS CP: modσy 1x10-15 apparently in reach, as seen from double-differences
GPS TAI P3: apparently the same instability for tau >= 2 days
R. Dach (AIUB), G. Petit (BIPM), L. Lorini (IMGC), P. Whibberley, R.Hlavac(NPL), T. Parker (NIST), J. Achkar, P. Uhrich (OP), A. Bauch (PTB):Time and Frequency Comparisons between fourEuropean Timing Institutes and NIST Using Multiple Techniques:EFTF 2005, Besancon
Time links existing between USNO and PTB
USNO PTB
GPS-related linkstwo-way links viatelecom satellites
multi-channel C/A codegeodetic time-transfer
(TAI-P3 and IGS) Ku-band (11-14 GHz)
X-band (7-8 GHz)
D. Piester, A. Bauch, T. Polewka, J. Becker (PTB)
A. McKinley, L. Breakiron, A. Smith, B. Fonville, D. Matsakis (USNO)
Motivation
Laboratory equipped with TWSTFT GPS CV single-channel linkTWSTFT GPS CV single-channel back-up linkTWSTFT by Ku band with X band back-up GPS CV multi-channel linkLaboratory equipped with dual frequency reception GPS CV multi-channel back-up linkGPS CV dual frequency linkGPS CV dual frequency back-up link
North America Europe Asia
South America Africa Oceania
USNO
ONBA TCC IGMA ONRJ CSIR
CNMP CNM
NRC
APL
ROA DTAG BEV AOS PL LT SU NIMB
CRL
AUS
PTB
IEN
OP
NPL
VSL
ORB DLR IFAG CH LDS JV SP
NPLI
INPL
SMU
NMC
UME
TP
OMH
CAO
NIST
NTSCJATC
MSL
SCL
NMIJ
TL
KRIS
SG
NIMT NMLS BIRM
NIM
NAO
ORGANIZATION OF THE INTERNATIONAL TIME LINKS March 2004
The link between USNO and PTB connects almost one half of theclocks contributing to TAI
Long-term link characteristics
Differencebetweendaily data of Ku-band and X-band
best-fitsine function
period370 days
amplitude0.6 ns
Calibration of Time Link USNO – PTB
Results of repeated calibrations using travelling X-band station
1.1.2002 1.1.2003 1.1.2004 1.1.2005 1.1.2006-4-3-2-101234
-4-3-2-101234
diff
eren
tial c
alib
ratio
n (n
s)
date
X-band
Ku-band
Results of USNO – PTB link
1) Link Characteristics - variations of 0.6 ns with one year period
2) Calibration - combined uncertainties below 1 ns achievable
- investigation of correlation with temperature variations
- operation of two low-noise links in parallel sufficient
Possible improvements with microwave links
• Use higher chip-rate (bandwidth limitation)
• Use dedicated transponders
• Present performance is not limited by microwave technology-but by not implementing the best possible existing technology
• However ...
T [s]
1 10 100 1000
σ y o
f diff
eren
ce fr
eque
ncy
2x10-16
4x10-16
6x10-168x10-16
10-15
2x10-15
4x10-15
E. Peik, T. Schneider, Chr. Tamm,J. Phys. B: At. Mol. Opt. Phys 39,145 (2006)
Stability of an Yb+
single ion clock at PTB
Time Transfer by Laser Link
Laser station emits asynchronous, short light pulses (~ 20 ps FWHM)towards the satellite. Retro-reflecting corner-cubesreturns a fraction of thereceived photons back to thestations. The station records the start (tS) and return (tR) time of each light pulse.
Time Transfer by Laser Link
1. Lasso:proposed in 1972 and launched in 1988 on Meteosat P2.A first optical time transfer had been successfullyachieved in 1992 betw. OCA, France and Mac Donald, USA.
2. T2L2:• first proposed in 1996 to fly on the Russian space station MIR• later accepted by ESA in the framework of the ACES programscheduled on the ISS; descoped in 2001
• now payload on the Jason-2 space vehicle, whichwill be launched in mid 2008 for a 5 years long mission.
Expected performances are in the 100ps range for accuracy, with an ultimate stability better than 1ps over 1000s (onepass) and than 10ps over one day.
Frequency Transfer via TelecommunicationFibre Network
Frequency standard
Frequency standard
Fibrenetwork
Transfer laser1,5 µm
Transfer laser1,5 µm
Frequency comb Frequency comb
Opticalfrequency
comparison
1 10 100 1k 10k 100ks10-18
10-17
10-16
10-15
10-14 ALLAN STANDARD DEVIATION of FREQUENCY
86 km User End cw Laser Link 86 km LLink Modulated Laser ( with Scrambler)
σy( 2
, τ )
integration time
Two-way Fibre Link
G. Santarelli, H. Schnatz, B. Lipphardt, G. Grosche, Nov. 2006 @ SYRTE
Vision: European Fibre Network
NPLLondon
UniHannover
PTBBraunschweig
UniBerlin
MPQGarching
INRIM Turin
Telecom Fibre Network
Sr, Yb
Mg
H
Sr, Yb+
SYRTE- LPLParis
Sr, Yb+
ESA
Conclusions
• TWSTFT on transcontinental links approaches a fractionalinstability of 10-15 per day
• With repeated calibrations < 1ns have been demonstrated
• Better technology is in general available, that could improvestability by an order of magnitude
• The microwave technology does not seem capable to supportthe requirements of the optical clocks
• Optical satellite links are in an experimental status
• Terrestrial optical fibre links are going to be explored
Help fromA. Bauch, D.Piester, H. Schnatz, E. Peikis gratefully acknowledged