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S.Klimenko, March 2003, LSC Burst Analysis in Wavelet Domain for multiple interferometers LIGO-G030132-00-Z Sergey Klimenko University of Florida l Analysis.

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Presentation on theme: "S.Klimenko, March 2003, LSC Burst Analysis in Wavelet Domain for multiple interferometers LIGO-G030132-00-Z Sergey Klimenko University of Florida l Analysis."— Presentation transcript:

1 S.Klimenko, March 2003, LSC Burst Analysis in Wavelet Domain for multiple interferometers LIGO-G030132-00-Z Sergey Klimenko University of Florida l Analysis strategy l Data analysis pipeline  WaveMon veto generator (S.Klimenko, see LIGO note G020383-00-Z)  WaveBurst event generator (S.Klimenko, I.Yakushin) l Analysis algorithms l Some results for S1 l Summary & Plans

2 S.Klimenko, March 2003, LSC Analysis strategy l Triggers are generated independent for each IFO l GW candidates are generated on the final coincidence step GW events coincidence VETO ETG: tfcluster, slope, power VTG: glitch monitors ifo1 auxiliary channels VETO ETG: tfcluster, slope, power VTG: glitch monitors Ifo1,… auxiliary channels

3 S.Klimenko, March 2003, LSC event trigger generators l pixels produced by artifacts are clustering together - very powerful idea behind the Time-Frequency cluster analysis l use coincidence to enhances it. l coincidence is used before the events are generated  approach often used in HEP. data conditioning: wavelet transform, rank statistics, pixel selection channel 1 data conditioning: wavelet transform, rank statistics, pixel selection channel 2,… “coincidence” event generation event generation WaveBurst/WaveMon data conditioning: Fourier transform, Gaussian statistics, pixel selection channel 1 event generation TFCLUSTER

4 S.Klimenko, March 2003, LSC Wavelet Transform l Optimize search by selecting wavelet type & decomposition tree l detail coefficients d i represent data in different frequency bands  df = f/2, f/4, f/8, ….. - dyadic, df = f/n, - linear basis wavelet transform tree d0d0 d1d1 d2d2 a db8

5 S.Klimenko, March 2003, LSC wavelet time-scale(frequency) plane l For short (therefore broadband) bursts dyadic WT should be good. l For long signals, like inspirals, binary WT could be optimal l Several wavelet transforms are implemented in the datacondAPI l Currently used in WaveBurst:  interpolating bi-orthogonal, Daubechies, Simlets  binary wavelet tree (linear frequency scale)

6 S.Klimenko, March 2003, LSC Percentile Transform l given a sample with amplitude A, define its percentile amplitude as a=1/f, where f is fraction of samples in the population with absolute value of amplitude greater then | A| l Equivalent to calculation of rank statistics  non-parametric l percentile amplitude distribution function: P(a)=1/a 2  the same for all wavelet layers

7 S.Klimenko, March 2003, LSC raw  percentile TF plots H2:LSC-AS_Q H2:IOO-MC_F

8 S.Klimenko, March 2003, LSC 10% H2:LSC-AS_Q 224-240 Hz 10% Percentile Thresholding Rule l threshold on percentile amplitude l select a certain fraction of samples (set T-F occupancy) l don’t care about the data distribution function l one possible way of “de-noising of wavelet data”

9 S.Klimenko, March 2003, LSC Coincidence Rules accept reject l Given local occupancy O i (t,f) in each channel, after coincidence the cluster occupancy is l For strict coincidence O i (t,f) = p 2 for random pixels produced by noise. for example if p=0.1, average occupancy after coincidence is 0.01 l WaveBurst can use various coincidence policies  allows customization of the pipeline for specific burst searches.

10 S.Klimenko, March 2003, LSC strict coincidence l coincidence TF plot for LSC-AS_Q && IOO-MC_F l coincidence allows  set a low threshold at the previous (thresholding) step  “build” clusters with known false alarm rate, determined by random clustering of pixels

11 S.Klimenko, March 2003, LSC Cluster Analysis Cluster Parameters size – number of pixels in the core volume – total number of pixels density – size/volume amplitude – maximum amplitude power - wavelet amplitude/w50 energy - power x size asymmetry – (#positive - #negative)/size likelihood – log(  A i ) neighbors – total number of neighbors frequency - core minimal frequency [Hz] band - frequency band of the core [Hz] time - GPS time of the core beginning interval - core duration in time [sec] cluster core positive negative Cluster halo cluster – T-F plot area with high occupancy

12 S.Klimenko, March 2003, LSC ‘orthogonal’ data sets l WaveMon/WaveBurst generate clusters of three types:  candidate clusters  potential GW bursts  off-time clusters (due to random coincidence of glitches)  veto tuning  “false alarm” clusters (due to random clustering of noise)  threshold settings quiet channel hot channel WaveMon rates for coincidence with H2:LSC-AS_Q S1 data blue – candidates red – off-time green - random

13 S.Klimenko, March 2003, LSC selection cuts: cluster likelihood l L threshold can be set a priori based on the false alarm rate  does not need tuning  perfect for real time processing  Only L threshold is applied at run time  ETG output rate ~0.2Hz SG strain=5e-18 100-2000 Hz

14 S.Klimenko, March 2003, LSC selection cuts: cluster “energy” For Gaussian noise E=  2 l Energy cut is set based on the false alarm rate and it is used for post-processing event selection w i – wavelet amplitude w 0 – distribution median w 50 – median of |w i -w 0 | S1 playground Software injections strain=5e-18

15 S.Klimenko, March 2003, LSC VETO l After applying selection cut, remaining events are suppose to be removed with vetoes l Veto events can be generated by DMT monitors and by ETGs itself. l Off-time data set (red dots) is used for selection of effective veto channels nothing to veto for S1 playground data, except for frequency band<150Hz But veto will be very important for large data sets work in progress on optimization of veto strategy no whitening

16 S.Klimenko, March 2003, LSC Other issues l Simulation study using injected bursts:  pipeline consistency check.  efficiency study for different coincidence policies using bursts injected randomly in time and with random delay between detectors. l X-correlation between burst candidates found in two detectors. Could be significant enhancement of the search pipeline. (see Malik’s talk)

17 S.Klimenko, March 2003, LSC Conclusion & Plans l WaveBurst ETG  produces GW burst candidates for a coincidence of two detectors  uses non-parametric statistics  allows a priori threshold settings for the on-line operation.  produce event triggers with known false alarm rate l WaveMon monitors the detector glitch performance  Can help identify the source of glitches in the GW channel by looking at frequency content and correlation with auxiliary channels  produces veto triggers l Plans  Use S1 as a playground for WaveBurst pipeline.  Process S2  Preparations for S3


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