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S5 Q Pipeline Status

The S5 Q Pipeline is used to search for untriggered bursts in S5 data through April 3, 2006. This analysis consists of double coincident and triple coincident searches using H1H2 and L1 triggers. Upper limits are determined using the loudest event statistic.

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S5 Q Pipeline Status

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  1. S5 Q Pipeline Status Shourov K. Chatterji Caltech LIGO Scientific Collaboration meeting MIT 2006 November 5

  2. S5 Q Pipeline search • The Q Pipeline is being applied to search for untriggered bursts in S5 data through 2006 April 3. • There are two primary components of this analysis • H1H2 double coincident search for combined excess signal energy followed by H1H2 null stream consistency test • H1H2L1 triple coincident search for time frequency coincidence between H1H2 triggers and L1 triggers • Upper limits will be determined using the loudest event statistic • The loudest N events will be followed up QScans and a fully coherent follow-up if data is available from a sufficient number of detectors LSC meeting 2006 November 5

  3. Q Pipeline • Multiresolution time-frequency search for statistically significant excess signal energy • Projects whitened data onto an overlapping basis of sinusoidal Gaussians characterized by central time, central frequency, and Q (ratio of central frequency to bandwidth) • The template bank is constructed using a maximum mismatch approach similar to the matched filtering approach • The search is equivalent to a matched filter search for waveforms that are sinusoidal Gaussians after whitening • The reported normalized energy is measure of event significance and is simply twice the squared SNR that would be reported by a matched filter search LSC meeting 2006 November 5

  4. H1H2 Null stream veto • The collocated H1H2 search has two components • H+: The optimal linear combination of H1 and H2 that maximizes the SNR of potential signals • Weighting factors are inversely proportional to power spectral density in each frequency bin • Normalized energy, Z+, is twice the quadrature sum of SNR in both detectors • H-: The H1 – H2 null stream, which should be consistent with noise for real gravitational-waves • To avoid calibration uncertainties, test normalized energy, Z-, against that expected null stream normalized energy, Z0, assuming incoherent glitches in the two detectors • Z- > a + b Z0 LSC meeting 2006 November 5

  5. Analysis code • The QScan and QPipeline codes have been merged into a single code base, which is now available in the LSC MatApps CVS repository [links: code, documentation] • This code base is now installated on most LSC computing clusters and LIGO laboratory general computing networks. • Running QPipeline is now as simple as running QScan ssh ldas-pcdev1.ligo.caltech.edu mkdir –p ~/qpipelinetest cd ~/qpipelinetest ~shourov/qscan/bin/qpipeline.sh \ 843214931 843215031 \ @H1H2-collocated @S5 . It’s easy!Try it now! LSC meeting 2006 November 5

  6. Summary of livetime and duty cycle H1 H1H2 90.1(60.1%) 3.3(2.2%) 5.1(3.4%) 34.4(22.9%) 55.8(37.2%) 12.7(8.5%) 10.2(6.8%) 7.1(4.7%) H2 L1 Livetime in days through April 3, 2006 Duty cycle relative to start of S5 at LHO LSC meeting 2006 November 5

  7. Data quality and vetoes • The following data quality flags were used to define the segment lists for trigger generation • No other data quality flags have been applied. • No auxiliary channel vetoes have been applied. OUT_OF_LOCK OUT_OF_SCIENCE_MODE PRE_LOCKLOSS_120 MISSING_RDS_C02_LX Injection LSC meeting 2006 November 5

  8. Search parameters channelNames: {'H1:LSC-STRAIN', 'H2:LSC-STRAIN'} frameTypes: {'H1_RDS_C02_LX', 'H2_RDS_C02_LX'} timeShifts: [+0 -1] injectionNames: {'H1:GW-H', 'H2:GW-H'} injectionTypes: {'SG2_S5_A', 'SG2_S5_A'} injectionFactors: [0.5 0.5] reSampleFrequency: 4096 blockDuration: 64 minimumBlockOverlap: 8 qRange: [4 64] frequencyRange: [64 1024] maximumMismatch: 0.2 analysisMode: 'collocated' outlierFactor: 2.0 falseRate: 1e0 maximumSignificants: 1e5 maximumTriggers: 1e3 durationInflation: 1.0 bandwidthInflation: 1.0 Using h(t) data Using burst MDCs Search space LSC meeting 2006 November 5

  9. Post-processing parameters • High threshold veto • H+ events are excluded if they fall within two seconds of very inconsistent tiles (Z- > 128 + 0.1 Z0) • Low threshold veto • H+ events are excluded if they overlap inconsistent tiles (Z- > 18 + 0.05 Z0). • Low frequency, low Q cut • A significant fraction of all glitches are observed to fall in the lowest frequency, lowest Q template. • H+ events are excluded if they have a central frequency less than 100 Hz and a Q less than 14. LSC meeting 2006 November 5

  10. Trigger production • Trigger production and post-processing is visible online LSC meeting 2006 November 5

  11. Distribution of H1H2 significance Loudest event Z+ = 176 LSC meeting 2006 November 5

  12. Loudest H1H2 event • Loudest event is low Q burst in H1 • No clear glitch in H2 • Why did this pass the H1H2 null stream veto? • Potential room for improved veto tuning? H1 H2 LSC meeting 2006 November 5

  13. Efficiency for sinusoidal Gaussians LSC meeting 2006 November 5

  14. Efficiency for sinusoidal Gaussians LSC meeting 2006 November 5

  15. Efficiency for Gaussians LSC meeting 2006 November 5

  16. Efficiency for white noise bursts LSC meeting 2006 November 5

  17. Predicted (“time lag”) upper limits Decreased efficiency Increased livetime Crossover at 7e-22 and 0.08 events per day LSC meeting 2006 November 5

  18. Outlook • Further tuning will likely improve performance • Anything that eliminates loud events will improve the resulting upper limit • Triple coincidence (at the expense of livetime) • Application of data quality flags and vetoes based on auxiliary or environmental channels • Concern about potential zero lag H1H2 surprise • Use S4 as a playground data set • Trigger production complete at 17 different time lags including zero lag • Use one day of S5 as a playground data set • Once tuning is complete, the box will be opened for the analysis through April 3. LSC meeting 2006 November 5

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