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A Waveform Consistency Test for Binary Inspirals using LIGO data

A Waveform Consistency Test for Binary Inspirals using LIGO data. Andres C. Rodriguez Gabriela González (Louisiana State University). Peter Shawhan (LIGO | Caltech) Evan Oshsner (University of Maryland). LSC Inspiral Analysis Working Group LIGO-G050236-00-Z

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A Waveform Consistency Test for Binary Inspirals using LIGO data

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  1. A Waveform Consistency Test for Binary Inspirals using LIGO data Andres C. Rodriguez Gabriela González (Louisiana State University) Peter Shawhan (LIGO | Caltech) Evan Oshsner (University of Maryland) LSC Inspiral Analysis Working Group LIGO-G050236-00-Z American Physical Society April Meeting 4.16.05

  2. LIGO Observatories Hanford: two interferometers in same vacuum envelope (4km(H1), 2km(H2)) Livingston: one interferometer (4km(L1)) American Physical Society April Meeting 4.16.05 02

  3. Template based Matched Filtering Template based Matched Filtering • Data stream searched using matched filtering between • data & template waveform. • Transform data to frequency domain : s(f) • Calculate template in frequency domain: h(f) s(t) = n(t) + h(t) ~ ~ American Physical Society April Meeting 4.16.05 03

  4. Template based Matched Filtering • Signal to Noise (): • 2: American Physical Society April Meeting 4.16.05 04

  5. Template based Matched Filtering - Thresholds • Signal to Noise (): • 2 : • » really: • So if  > * and r2 < r2* --> inspiral “trigger”  > threshold (* ) < threshold (r2*) American Physical Society April Meeting 4.16.05 05

  6. Simulated Inspiral (Injection) Injection * SNR r2* r2 -2 0 +2 time (s) to inferred coalescence American Physical Society April Meeting 4.16.05 06

  7. Injection vs. Trigger Injection Trigger SNR r2 -2 0 +2 time (s) to inferred coalescence American Physical Society April Meeting 4.16.05 06

  8. Injection vs. Trigger Injection Trigger r2 -2 0 time (s) to inferred coalescence American Physical Society April Meeting 4.16.05 07

  9. The Test • Use the r2 time series as a method to search for excess noise • Impose a “looser” r2 threshold than the search employs • » Count the number of time samples above a given • threshold in a time interval before inferred coalescence • » Count the number of threshold crossings • Time interval “window” chosen to be 2 seconds • Do my triggers behave like software, hardware injections? • » yes ->> keep • » no ->> veto American Physical Society April Meeting 4.16.05 08

  10. 2 , r2 distribution log10(counts) 0 200 70 r2 0 2 American Physical Society April Meeting 4.16.05 09

  11. 2 , r2 distribution log10(counts) 0 40 12 r2 0 2 American Physical Society April Meeting 4.16.05 09

  12. Injection vs. Trigger Crossings = 0 Time above Threshold = 0 sec Crossings = 52 Time above Threshold = 0.9 sec r2 looser r2 threshold American Physical Society April Meeting 4.16.05 10

  13. Preliminary Results for H1 Injections + Playground Data r2 threshold = 10 window H1 Injections Time above r2 threshold (ms)  American Physical Society April Meeting 4.16.05 11

  14. Preliminary Results for H1 Injections + Playground Data r2 threshold = 10 H1 Injections Time above r2 threshold (ms)  American Physical Society April Meeting 4.16.05 11

  15. Preliminary Results: H1 Injections + Playground Data possibly vetoed r2 threshold = 10 Crossings < 2 H1 Injections Triggers Time above r2 threshold (ms)  American Physical Society April Meeting 4.16.05 11

  16. Summary and Plans • Preliminary testing r2 thresholds set to 6, 8, & 10. • The test would be able to eliminate many of our loudest • false triggers --> reduces false alarm rate. • Additional tuning using S3 Hardware Injections and • testing on S3 playground data from L1,H2. • Will be incorporated into S3, S4 BNS search, and future • online analysis. American Physical Society April Meeting 4.16.05 12

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