Thermal Noise performance of advanced gravitational wave detector suspensions Alan Cumming, on...
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Transcript of Thermal Noise performance of advanced gravitational wave detector suspensions Alan Cumming, on...
Thermal Noise performance of advanced gravitational wave detector
suspensions
Alan Cumming, on behalf of the University of Glasgow Suspension Team
5th April 2011
2
Overview
• Silica suspension design for aLIGO
• Prototype aLIGO suspension
• Thermal noise performance and loss modelling
• Current status
• Future work
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aLIGO Monolithic Silica Stage
Steel wires
Penultimate mass
‘Ear’
Silica fibres
End/input test mass
‘Ear’
Requirement: 10-19m/Hz @ 10Hz
Upper metal masses (22kg
masses)
Blade springs
Lower Monolithic silica stage
(40kg masses)
Prototype Suspension, MIT
• Laser pulled silica fibres
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A. Heptonstall et al., Rev. Sci. Inst. 82, 011301 (2011) Fibres laser welded to ears
Complete suspension
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Ear
FibreNeck
Stock Weld
Finite Element Analysis
• Use FEA to predict energy stored in the suspension elements and the dissipation dilution, D
elastic
total
E
ED
A. Cumming et al., Class. Quant. Grav., 215012, 2009,A. Cumming et al., Class. Quant. Grav., in preparation,
2011.
Ear Horn
Modelling the suspension loss
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• Internal friction described by the mechanical loss of the system • For a suspension this originates from various different mechanisms in the fibre ends:
• Modelling with FEA gives
Surface loss, surf
Bulk loss, bulk
Weld loss, weld
Thermoelastic loss, th
weldbulksurfthtotal
1 D
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Modelling comparison with measured
A. Cumming et al., Class. Quant. Grav., in preparation, 2011
• Measurement of horizontal noise difficult
• Modelling compared by predicting loss of violin modes
of suspension fibres
• Measured on MIT prototype suspension
• Gives good confidence in modelling technique
Violin mode FEA Frequency (Hz)
Measured
Frequency (Hz)
Projected loss from
FEA model Measured loss
Fundamental 511 511,520 1.50 x 10-9 1.61 x 10-9
1st harmonic 1017 1020 1.75 x 10-9 2.16 x 10-9
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aLIGO Final Stage Noise (Single Test Mass)
10-19m/Hz @ 10Hz
A. Cumming et al., Class. Quant. Grav., in preparation, 2011
99
Current status and future work
• Suspension design for aLIGO now finalised
• Preparation for the start of manufacture of production suspensions for first installations into the LIGO instruments is currently ongoing
• First installations timetabled for summer 2011
• Studies already ongoing on methods to further increase sensitivity for enhancements to aLIGO using the FEA modelling techniques
• Application of modelling to future third generation detectors using different materials and possibly cooled to cryogenic temperatures
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Thermal Noise Model
22224
22 4
ototalo
totaloB
m
Tkx
hornweldfibretotal
1
D
• Use the following loss terms to model the welds, ear horns and fibres
n totalelastic
n2
totalelastic
21
totalelastic
1
E
E
E
E
E
E
2
2
ticthermoelas1
YC
YTo
d
h s 8surface
77.011bulk 102.1 f
7weld 108.5
A.M. Gretarsson et al., Phys. Rev. A, 2000 G. Cagnoli and P.A. Willems, Phys. Rev. B, 2002P.A. Willems, T020003-00M.Barton et al., T080091-00-KA. Heptonstall et al., Phys. Lett. A, 354, 2006A. Heptonstall et al., Class. Quant. Grav, 035013, 2010