allegro g050208-00-z lsc, livingston 23 march, 2005 1 calibration for the allegro resonant detector...
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G050208-00-Z LSC, Livingston 23 March , 2005
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ALLEGRO
Calibration for the ALLEGRO resonant detector -- S2 and S4
Martin McHugh, Loyola University New Orleans
Warren Johnson, Louisiana State University
with the ALLEGRO group, Stochastic Sources Subgroup
G050208-00-Z LSC, Livingston 23 March , 2005
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ALLEGRO
Outline
• Motivation, background
• Signal flow diagram, transfer function equations
• Discussion of calibration measurements
• Recent mysteries
• summary
G050208-00-Z LSC, Livingston 23 March , 2005
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ALLEGRO
Motivation
• Provide input to stochastic background analysis using ALLEGRO and LLO (John Whelan’s talk earlier this week)
• Unlike an event list based search, a coherent search such as this requires a phase consistent response function for the detector signal path
G050208-00-Z LSC, Livingston 23 March , 2005
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ALLEGRO
ALLEGRO schematic
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ALLEGRO
Signal path
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ALLEGRO
€
˜ z v ( f − f r ) = A( f ) ˜ v S ( f ) = aLe i(td 2π ( f − fr ))e−iφ ˜ v S ( f )
€
˜ F ( f ) = J( f ) ˜ h ( f ) = 4MLf 2 ˜ h ( f )
€
˜ x ( f ) = G( f ) ˜ F ( f )
= α1
f p2 − f 2 +
if p f
Qp( )−
1
fm2 − f 2 + ifm f
Qm( )
⎛
⎝
⎜ ⎜
⎞
⎠
⎟ ⎟˜ F ( f )
€
˜ I ( f ) = K ⋅ ˜ x ( f ) =IDC
g
⎛
⎝ ⎜
⎞
⎠ ⎟˜ x ( f )
€
˜ v S ( f ) = Z ⋅ ˜ I ( f )
€
˜ z c ( f − f r ) = D ⋅ ˜ z v ( f − f r )
Form of each Transfer Function€
˜ F C ( f ) = H ˜ v e ( f ) =CcVDC
gc
˜ v e ( f )
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ALLEGRO
Need to determine --
• Mode frequencies and Q’s -- fm , fp , Qm , Qp
• overall scale -- in practice we measure is mechanical gain -- includes
‘tuning factor’
• Lock-in amplifier parameters -- gain, filter delay and phase shiftAlso need to know the phase of
the lock-in reference oscillator
€
⋅K ⋅Z
So in practice the calibration amounts to --
€
˜ h ( f − fr ) =˜ z C ( f − f r )
J( f )G( f )KZA( f − f r)D
Inverse fft then gives
€
h H (t) complex heterodyned strain time series
G050208-00-Z LSC, Livingston 23 March , 2005
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ALLEGRO
New calibrator installed between S2 and S4 -- known transfer function
• One plate of capacitor is tightly coupled to bar.
• Other plate is weakly coupled to the bar, so acts like a free mass.
• Both plates electrically isolated.
Rest of detector unchanged -Measurements will apply to S2
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ALLEGRO
The calibrator mounted on the bar
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ALLEGRO
Transfer function - white noise excitation to measured output
measurements from 20 March 2004 -- excitation measured through lock-in and A/D plotted here we have
€
TF = H ⋅G( f ) ⋅K ⋅Z
gives us the overall scale -
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ALLEGRO
Band-limited white noise injection -- recorded directly and through lock-in/anti-aliasing filters
Lock-in/ filter measurements
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ALLEGRO
Compare fourier coefficients
Lock-in/filter introduces an 11ms delay and 18 degree phase shift
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ALLEGRO
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ALLEGRO
Calibration lineCalibration line
Detector resonancesDetector resonances
Extra mechanical resonancesExtra mechanical resonances
Raw data
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ALLEGRO
Calibrated strain spectrum from S4
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ALLEGRO
Stability of calibration -- calibration line tracked through S2
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ALLEGRO
• Discrepancy between white noise injection data sets discovered to be due to change in polarity of DC
bias applied to calibrator (?!)
• Two mysteriesNuisance mode at 885 Hz -- relative phase changes
with DC bias polarityApparent offset in DC bias voltage on calibrator
A Problem
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ALLEGRO
Transfer function magnitude, white noise injection --blue curve +3.99VDC nominal biasred curve -3.99VDC nominal bias
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ALLEGRO
… now flip the plate to which the voltage is applied
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ALLEGRO
we can certainly model extra mechanical modes -- but the phase flip is a mystery
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ALLEGRO
837Hz calibration line strength vs. calibrator bias
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ALLEGRO
Summary
• We have calibrated h(t) for S2 data set • Hardware injections done for E12, S4 -- good news
we are able to extract coherent signal between L1 and A1 (see Sukanta’s earlier talk)
• Analyze burst injections done to determine overall sign of the calibration
• Need to investigate calibrator behavior with post S4 measurements -- be sure there is no problem with overall scale determination