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Martin McHugh Loyola University New Orleans on behalf of the ALLEGRO group

Generating time domain strain data ( h ( t )) for the ALLEGRO resonant detector or calibration of ALLEGRO data. Martin McHugh Loyola University New Orleans on behalf of the ALLEGRO group http://sam.phys.lsu.edu/. Outline. Motivation Signal flow diagram, transfer function equations

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Martin McHugh Loyola University New Orleans on behalf of the ALLEGRO group

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  1. Generating time domain strain data (h(t)) for the ALLEGRO resonant detectororcalibration of ALLEGRO data Martin McHugh Loyola University New Orleans on behalf of the ALLEGRO group http://sam.phys.lsu.edu/ GWDAW-9, Annecy 16 December , 2004

  2. Outline • Motivation • Signal flow diagram, transfer function equations • Discussion of calibration measurements • Noise curves, stability • future GWDAW-9, Annecy 16 December , 2004

  3. Motivation • LSC stochastic background analysis using S2 data from ALLEGRO and LIGO Livingston (see John Whelan’s talk later today) • Unlike an event list based search, a coherent search such as this requires a phase consistent response function for the detector signal path GWDAW-9, Annecy 16 December , 2004

  4. ALLEGRO schematic GWDAW-9, Annecy 16 December , 2004

  5. Signal path GWDAW-9, Annecy 16 December , 2004

  6. Form of each Transfer Function GWDAW-9, Annecy 16 December , 2004

  7. Need to determine -- So in practice the calibration amounts to -- • 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 shift • Also need to know the phase of the lock-in reference oscillator Inverse fft then gives complex heterodyned strain time series GWDAW-9, Annecy 16 December , 2004

  8. transducer current changed temperature fluctuations S2 data -- 2003 GWDAW-9, Annecy 16 December , 2004

  9. New calibrator • 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. GWDAW-9, Annecy 16 December , 2004

  10. The calibrator mounted on the bar GWDAW-9, Annecy 16 December , 2004

  11. 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 gives us the overall scale -  GWDAW-9, Annecy 16 December , 2004

  12. GWDAW-9, Annecy 16 December , 2004

  13. Lock-in measurements Band-limited white noise injection -- recorded directly and through lock-in/anti-aliasing filters GWDAW-9, Annecy 16 December , 2004

  14. Compare fourier coefficients Lock-in/filter introduces an 11ms delay and 18 degree phase shift GWDAW-9, Annecy 16 December , 2004

  15. GWDAW-9, Annecy 16 December , 2004

  16. Calibration line Detector resonances Extra mechanical resonances GWDAW-9, Annecy 16 December , 2004

  17. Calibrated strain spectrum from S2 GWDAW-9, Annecy 16 December , 2004

  18. Stability of calibration GWDAW-9, Annecy 16 December , 2004

  19. Summary, future • We have calibrated h(t) for S2 data set at level • Currently stored in Matlab files, plan to put these data into frames • detector much more stable now, should continue through S4 • will determine overall sign • hardware injections are planned GWDAW-9, Annecy 16 December , 2004

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