THE LISA GRAVITATIONAL WAVE MISSION
Edward Mitchell
March 2010
THE LISA GRAVITATIONAL WAVE MISSION Edward Mitchell March 2010 - - PowerPoint PPT Presentation
THE LISA GRAVITATIONAL WAVE MISSION Edward Mitchell March 2010 Gravitational Waves 2 Radiated by asymmetric changes in mass distributions (quadrupole moment or higher) Transverse, area preserving periodic strain in spacetime h10
Edward Mitchell
March 2010
Radiated by asymmetric changes in mass
Transverse, area preserving periodic strain in
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Edward Mitchell March 2010
Appear as time-dependent tidal forces in free-falling
Fractional change in proper distance: Strain amplitude of binary source approximated as: Observation of increasing binary orbital frequency
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Edward Mitchell March 2010
High power, predictable sources radiate below
Terrestrial gravity gradient/seismic noise limits earth
LISA target frequency range: 10-4-10-1Hz
Galactic binaries and extragalactic supermassive black
Laser interferometry – frequency analysis of phase
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Edward Mitchell March 2010
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Edward Mitchell March 2010
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Test mass follows geodesic path
TM position detected by
Micro-Newton thrusters maintain
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Edward Mitchell March 2010
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Optical path noise
Eg. Laser shot and phase noise Mimics change in arm length
Acceleration noise
Real arm length changes due to spurious forces Dominates at low frequency (f<2mHz), scaling as 1/f A major component is due to Coulomb and Lorentz forces
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Edward Mitchell March 2010
Galactic Cosmic Rays
Particles are
GCRs have nearly
SEP events (flares,
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[Grimani et al. Class. Quantum Grav. 21 (2004) S629-S633]
E<100MeV/n Primaries do not reach
test mass (TM)
100-400MeV/n Primaries stop in TM 400-2000MeV/n Primaries pass through,
secondary protons stop in TM
E>2000MeV/n Primary & secondary
protons pass though, secondary electrons stop
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Edward Mitchell March 2010
Test mass charging modelled with GEANT
Edward Mitchell March 2010
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Technology
Single spacecraft
Observe charging
LISA Technology Package [ESA]
UV photoelectron emission to maintain <105e
Two discharge modes: rapid/continuous
Charge fluctuations in time domain have coherent
Minimise through continuous discharge, matching
Charge rate varies due to stochastic arrival of
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Edward Mitchell March 2010
Edward Mitchell March 2010
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Measure and
Charging shot noise
Expected to exceed
Noise resulting from a net charging rate, for 1 day integration period, matching rates to ±10es-1 and maintaining Q<105e Dashed line = largest coherent Fourier component Red line = LISA noise target Blue line = LISA Pathfinder noise target
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Use radiation monitor to
Try to characterise transfer
Develop radiation monitors
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Edward Mitchell March 2010