Title: A particle monitor for LISA Pathfinder and Gravity Probe-B gyroscope charging in LEO
1A particle monitor for LISA Pathfinder and
Gravity Probe-B gyroscope charging in LEO
- Peter Wass, Henrique Araújo, Tim Sumner
- Imperial College London, UK
- Mokhtar Chmiessani, Alberto Lobo,
- IFAE IEEC, Barcelona, Spain
- Lenny Sapronov, Sasha Buchman
- Stanford University, California, USA
2Talk outline
- LISA and LISA Pathfinder
- Previous GEANT work
- LISA Pathfinder radiation monitor definition
- Radiation monitor simulations
- Conclusions
- Gravity Probe B
- Gyroscope charging simulations and data
- Proton monitor simulations and data
- Conclusions
3LISA and LISA Pathfinder
- Laser interferometer space antenna for detecting
gravitational waves in space - 3 spacecraft each with 2 free-floating test
masses - 5 million km arm-length
- 1 AU orbit
- Launch 2014
- LISA Pathfinder
- Drag-free technology demonstrator for LISA
- 1 spacecraft 2 test masses
- 30 cm baseline interferometer
- L1 Lagrange point orbit
- Launch 2008
4Test mass charging
- Science goals require almost perfect free falling
test masses (lt10-14ms-2Hz-1/2 at 1mHz) - Spurious non-gravitational forces arise if there
is excess charge on the test mass caused by
Solar particles (CME)
5Calculating TM charging
- Complex model of spacecraft
- Track all charged particles entering/leaving
test masses - Average charging rate stochastic charging
noise - Charging sensitivity to primary energy
6LISA Pathfinder radiation monitor
- Variations in charging can compromise science
goals of the mission - Want to measure the flux responsible for charging
- A particle monitor is proposed based on a
telescopic arrangement of PIN diodes. - 5-10 g/cm2 of shielding stops particles
Elt70-90MeV - Count rates sufficient to detect small
fluctuations in flux - Energy resolution to distinguish GCR and SEP
spectra.
7Simulations
- Simulate performance of the monitor using GEANT4
- Predict the count rates due to GCR flux and
during SEP events - Record deposited energy spectrum measured from
coincident hits in the PIN diodes.
8Results
- Particles with energy below 72 MeV can not
penetrate shielding - gt90 of particles with Egt120 MeV are detected.
- GCR (min) count rate of 7 counts/s from both
diodes
No noise Noise threshold
SEP alphas Isotropic 19.1 18.8
SEP alphas Coincident 0.97 0.95
GCR alphas Isotropic 7.4 7.2
GCR alphas Conincident 0.38 0.37
9Results
- The energy spectrum deposited in the diodes
during small SEP events can be distinguished in
measurement periods shorter than 1hr. - The average angular acceptance of the telescopic
configuration of diodes is 30 deg FWHM. - For particles with energies lt120 MeV the
acceptance is 15 deg.
10Conclusions and Future work
- According to simulations, the monitor fulfils all
requirements - 28 October 2005 - Radiation monitor testing at
PSI - Using 50-250MeV protons, measure
- Shielding cut-off
- Max count rates
- Angular dependence
- Diode degradation
11Gravity Probe B
- Aims to detect geodetic and frame-dragging
effects on free-falling gyroscopes in low earth
orbit - 600km polar orbit
- Gyroscopes accumulate charge from SAA
- GP-B payload also includes a high energy proton
monitor (30-500MeV)
12Simulations
- Use simulation code adapted from LISA/LISA
Pathfinder work - Simplified model of GP-B spacecraft concentric
shielding - Use orbit averaged proton spectra to calculate
charging rate - AP-8 solar maximum model
Feature Material Thickness (cm) g/cm2 Approx. Geometry
Outer vacuum shell Al 0.25 0.68 Sphere 200cm
Insulation/Silk Mesh MLI 0.270.1 0.52 Sphere 170cm
Radiation shields Al 0.20 0.54 Sphere 160cm
Main Tank Al 0.23 0.62 Sphere 155cm
Proton Shield Al 3.71 10.02 Sphere 32cm
Cryoperm shield Fe 0.10 0.87 Sphere 27.1cm
Probe vacuum shell Al 0.53 1.43 Sphere 26cm
Lead bag Pb 0.01 0.11 Sphere 25cm
Quartz block SiO2 (quartz) 2.50 5.50 Cylinder ?6.1cm h16cm
Niobium shield Nb 0.05 0.43 Cylinder ?6 cm h16cm
Gyroscope housing SiO2 (quartz) 1.00 2.20 Sphere ?4cm
Gyroscope SiO2 (quartz) Solid 8.36 Sphere ?3.8cm
Total 31.3
13Results and data comparison
- The average charging rate, calculated from
simulations is 12.5e/s - Charging rate measured on orbit is 0.11mV/day or
8.0e/s
14GP-B proton monitor
- 414mm diameter silicon detectors
150µm-150µm-700µm -150µm - 2mm Tantalum shielding restricts angular
acceptance - 3mm aluminium window 45 deg view angle
- Energy determination from 700µm detectorrange
30-500MeV - GEANT model to simulate response of detector
- Compare with data to check flux model
15Simulation and data comparison
- Simulate average measured spectrum compare with
measurements from GP-B - Higher resolution data available for more
detailed analysis
16Conclusions and Future work
- Early results seem in good agreement
- Test other radiation models
- Charging/proton counts during solar particle
event - Difference between gyros?
- Simulate more complex geometry?
- Dedicated post-science phase measurements?