S.Klimenko, February 2004, cit ligo seminar Excess power method in wavelet domain for burst searches (WaveBurst) S.Klimenko University of Florida l Introduction l Wavelets l Time-Frequency analysis l Coincidence l Statistical approach l Results for S2 playground data l Simulation l Summary

S.Klimenko, February 2004, cit ligo seminar Newton-Einstein Theory of Gravitation Newton’s Theory 1666 “instantaneous action at a distance” Newton’s laws Einstein’s Theory 1915 “gravitational field action propagates at the speed of light” G +  g = 8  (G N /c 4 )T G is the Einstein tensor T is the stress-energy tensor

S.Klimenko, February 2004, cit ligo seminar gravitational waves time dependent gravitational fields come from the acceleration of masses and propagate away from their sources as a space- time warpage at the speed of light In the weak-field limit, linearize the equation in “transverse- traceless gauge” gravitational radiation binary inspiral of compact objects where h  is a small perturbation of the space-time metric

S.Klimenko, February 2004, cit ligo seminar GW strength Quadrupole radiation  monopole forbidden by conservation of E  dipole forbidden by mom. conservation For highly non-spherical source, like binary system with mass M and separation L 1 pc = 3 x m solar mass neutron stars  “Solar system” (1au) h~10 -8  Milky Way (20kpc) h~  Virgo cluster (15Mpc) h~  “Deep space” (200Mpc) h~  Habble distance (3000Mpc) h~ shakes planets by m

S.Klimenko, February 2004, cit ligo seminar Astrophysical Sources l Compact binary inspiral: “chirps”  waveforms are quite well described. Search with match filters. l Pulsars: “periodic”  GW from observed neutron stars (doppler shift)  all sky search l Cosmological Signals “stochastic”  x-correlation between several GW detectors l Supernovae / GRBs/ BH mergers/…: “bursts”  triggered search – coincidence with GRB/neutrino detectors  un-triggered search – coincidence of GW detectors

S.Klimenko, February 2004, cit ligo seminar GW interferometers Detection confidence Direction to sources AIGO GEO Virgo TAMA LIGO Livingston Hanford

S.Klimenko, February 2004, cit ligo seminar LIGO observatory

S.Klimenko, February 2004, cit ligo seminar Bursts Sources:  Any short transient of gravitational radiation.  Astrophysically motivated  Unmodeled signals -- Gamma Ray Bursts, …  “Poorly modeled” -- supernova, inspiral mergers l Analysis goals:  Establish a bound on rates  GW burst detection l Search methods  Excess power in time-frequency domain  Sudden change of the noise parameters, rise-time in time domain l In all cases: coincident observations among multiple GW detectors or with external triggers (GRBs, neutrinos). N: number observed events  (h): detection efficiency T: observation time

S.Klimenko, February 2004, cit ligo seminar l Exact waveforms are not known, but any information (like signal duration) could be valuable for the analysis (classification of the waveforms) Supernova Asymmetric core collapse gravitational waves asymmetric 30ms Zwerger,Muller

S.Klimenko, February 2004, cit ligo seminar Supernova rate SN Rate 1/50 yr - Milky Way 3/yr - out to Virgo cluster current sensitivity

S.Klimenko, February 2004, cit ligo seminar Inspiral Mergers Compact binary mergers l Expected merger detection rate ~40 higher then inspiral rate Flanagan, Hughes: gr-qc/ v  10Mo<M<200Mo (LIGO-I) 100Mo<M<400Mo (LIGO-II) events/year  very promising analysis

S.Klimenko, February 2004, cit ligo seminar S2 LIGO Sensitivity l Sensitive to bursts in  Milky Way  Magellanic Clouds  Andromeda  ……

S.Klimenko, February 2004, cit ligo seminar time-frequency analysis l Classify the GW “ecological calls” l Detect bursts with generic T-F properties in each class. l Characterize by “strength”, duration, frequency band,... Ecological calls of the Miniopterus australis the Macroderma gigas frequency time

S.Klimenko, February 2004, cit ligo seminar Wavelet basis Daubechies l basis  t   bank of template waveforms   0 - mother wavelet  a=2 – stationary wavelet Fourier wavelet - natural basis for bursts fewer functions are used for signal approximation – closer to match filter not local Haar local orthogonal not smooth local, smooth, not orthogonal Marr Mexican hat local orthogonal smooth

S.Klimenko, February 2004, cit ligo seminar Wavelet Transform decomposition in basis {  (t)} d4d4 d3d3 d2d2 d1d1 d0d0 a a. wavelet transform tree b. wavelet transform binary tree d0d0 d1d1 d2d2 a dyadic linear time-scale(frequency) spectrograms critically sampled DWT  fx  t=0.5 LP HP

S.Klimenko, February 2004, cit ligo seminar Wavelet time-scale(frequency) spectrogram H2:LSC-AS_Q LIGO data WaveBurst allows different tiling schemes including linear and dyadic wavelet scale resolution. for this plot linear scale resolution is used (  f=const)

S.Klimenko, February 2004, cit ligo seminar TF resolution d0d0 d1d1 d2d2 l depend on what nodes are selected for analysis  dyadic – wavelet functions  constant  variable  multi-resolution  select significant pixels searching over all nodes and “combine” them into clusters. wavelet packet – linear combination of wavelet functions

S.Klimenko, February 2004, cit ligo seminar Response to sine-gaussian signals wavelet resolution: 64 Hz X 1/128 sec Symlet Daubechies Biorthogonal  =1 ms  =100 ms sg850Hz

S.Klimenko, February 2004, cit ligo seminar WaveBurst analysis method detection of excess power in wavelet domain l use wavelets  flexible tiling of the TF-plane by using wavelet packets  variety of basis waveforms for bursts approximation  low spectral leakage  wavelets in DMT, LAL, LDAS: Haar, Daubechies, Symlet, Biorthogonal, Meyers. l use rank statistics  calculated for each wavelet scale  robust l use local T-F coincidence rules  coincidence at pixel level applied before triggers are produced  works for 2 and more interferometers

S.Klimenko, February 2004, cit ligo seminar “coincidence” Analysis pipeline bp  selection of loudest (black) pixels (black pixel probability P ~10% GN rms) wavelet transform, data conditioning, rank statistics channel 1 IFO1 cluster generation bp wavelet transform, data conditioning rank statistics channel 2 IFO2 cluster generation bp “coincidence” wavelet transform, data conditioning rank statistics channel 3,… IFO3 cluster generation bp “coincidence”

S.Klimenko, February 2004, cit ligo seminar Coincidence accept l Given local occupancy P(t,f) in each channel, after coincidence the black pixel occupancy is for example if P=10%, average occupancy after coincidence is 1% l can use various coincidence policies  allows customization of the pipeline for specific burst searches. reject no pixels or L <threshold

S.Klimenko, February 2004, cit ligo seminar Cluster Analysis (independent for each IFO) Cluster Parameters size – number of pixels in the core volume – total number of pixels density – size/volume amplitude – maximum amplitude power - wavelet amplitude/noise rms energy - power x size asymmetry – (#positive - #negative)/size confidence – cluster confidence neighbors – total number of neighbors frequency - core minimal frequency [Hz] band - frequency band of the core [Hz] time - GPS time of the core beginning duration - core duration in time [sec] cluster core positive negative cluster halo cluster  T-F plot area with high occupancy

S.Klimenko, February 2004, cit ligo seminar Statistical Approach l statistics of pixels & clusters (triggers) l parametric  Gaussian noise  pixels are statistically independent l non-parametric  pixels are statistically independent  based on rank statistics:  – some function u – sign function data: { x i }: |x k1 | < | x k2 | < … < |x kn | rank: { R i }: n n-1 1 example: Van der Waerden transform, R  G(0,1)

S.Klimenko, February 2004, cit ligo seminar non-parametric pixel statistics l calculate pixel likelihood from its rank: l Derived from rank statistics  non-parametric l likelihood pdf - exponential xixi percentile probability

S.Klimenko, February 2004, cit ligo seminar statistics of filter noise (non-parametric) l non-parametric cluster likelihood l sum of k (statistically independent) pixels has gamma distribution P=10% y single pixel likelihood

S.Klimenko, February 2004, cit ligo seminar statistics of filter noise (parametric) P =10% x p =1.64 y Gaussian noise l x: assume that detector noise is gaussian l y: after black pixel selection (| x |> x p )  gaussian tails Y k : sum of k independent pixels distributed as  k

S.Klimenko, February 2004, cit ligo seminar cluster confidence l cluster confidence: C = -ln (survival probability) l pdf(C) is exponential regardless of k. S2 inj non-parametric C parametric C S2 inj non-parametric C parametric C

S.Klimenko, February 2004, cit ligo seminar Coincidence Rates expect reduce background down to <20  Hz using post- processing selection cuts: triple event confidence, veto, … ifo pairL1-H1H1-H2H2-L1 triggers lock,sec rate, Hz double coincidence samples (S2 playground) raw triple coincidence rates triple coincidence: time window: 20 ms frequency gap: 0 Hz  1.10 ± 0.04 mHz off-time samples are produced during the production stage independent on GW samples GWDAW03

S.Klimenko, February 2004, cit ligo seminar “BH-BH merger” band raw triple coincidence rates off-time triple coincidence sample expect BH-BH mergers (masses >10 Mo) in frequency band < 1 kHz (BH-BH band) S2 playground background of 0.15 ± 0.02 mHz expect <1  Hz after post-processing cuts GWDAW03

S.Klimenko, February 2004, cit ligo seminar confidence of triple coincidence event l “arithmetic” l “geometric” S2 playground l Clean up the pipeline output by setting threshold on triple GC random noise glitches

S.Klimenko, February 2004, cit ligo seminar VETO l anti-coincidence with environmental & control channels  95% of LIGO data l generated with GlitchMon and WaveMon (DMT monitors) LIGO veto system is working ! address veto safety issue before use in the analysis L1 all 3 H2 H1 green – WaveBurst triggers with GC>1.7 after WaveMon VETO (~55 L1 channels) is applied dead time frac: ~5% veto efficiency: 76%

S.Klimenko, February 2004, cit ligo seminar WaveBurst false alarm summary l expect reduce background down to  <10  Hz for frequency band of Hz  < 1  Hz for frequency band of Hz by using post-processing selection cuts:  triple event confidence  veto l false alarm of 1 event per year is feasible with the use of the x-correlation cut. l expect <1 background events for all S2 (no veto)  WaveBurst is low false alarm burst detection pipeline l What is the pipeline sensitivity?

S.Klimenko, February 2004, cit ligo seminar Simulation l hardware injections l software injection into all three interferometers:  waveform name  GPS time of injection  , ,  - source location and polarization angle  T {L1,H1,H2} - LLO-LHO delays  F+{L1,H1,H2} - + polarization beam pattern vector  Fx {L1,H1,H2} - x polarization beam pattern vector l use exactly the same pipeline for processing of GW and simulation triggers. l sine-Gaussian injections  16 waveforms: 8-Q9 and 8-Q3  F+ {1,1,1}, Fx {0,0,0} l BH-BH mergers ( Mo)  10 pairs of Lazarus waveforms {h+,hx}  all sky uniform distribution with calculation {F+,Fx} for LLO,LHO  –duration f 0 -central frequency

S.Klimenko, February 2004, cit ligo seminar hardware injections SG injections [ 100Hz, 153Hz, 235Hz, 361Hz, 554Hz, 850Hz, 1304Hz 2000Hz ] good agreement between injected and reconstructed hrss good time and frequency resolution H1H2 pair

S.Klimenko, February 2004, cit ligo seminar detection efficiency vs hrss f o, Hz h 50%, Q h 50%, Q x Hz robust with respect to waveform Q

S.Klimenko, February 2004, cit ligo seminar timing resolution l time window >= 20 ms  negligible loss of simulated events (< 1%) S2 playground simulation sample  T =4ms 12% loss 1% loss

S.Klimenko, February 2004, cit ligo seminar Signal reconstruction reconstructed log10(hrss) mean amplitude frequency l Use orthogonal wavelet (energy conserved) and calibration.

S.Klimenko, February 2004, cit ligo seminar BH-BH merger injections l BH-BH mergers (Flanagan, Hughes: gr-qc/ v2 1997) duration : start frequency : bandwidth: l Lazarus waveforms (J.Baker et al, astro-ph/ v1) (J.Baker et al, astro-ph/ v1) all sky simulation using two polarizations and L & H beam pattern functions

S.Klimenko, February 2004, cit ligo seminar Lazarus waveforms: efficiency mass, Mo hrss(50%) x all sky search: hrss(50%)

S.Klimenko, February 2004, cit ligo seminar Lazarus waveforms: frequency vs mass l expected BH-BH frequency band – Hz

S.Klimenko, February 2004, cit ligo seminar WaveBurst pipeline status l WaveBurst ETG: stable, fully operational, tuned l S2 production: complete (Feb 8), ready to release triggers l Post-production  time, frequency coincidence: fully operational, tuned  trigger selection: fully operational, tuned  off-time analysis: ready to go l VETO analysis  feasible, good veto efficiency (87%)  need to finish production of WaveMon H1 and H2 triggers  requires cleaning-up veto sample and some tuning to reduce DTF  address more accurate veto safety with software injections l Simulation  All sky SG,BH-BH mergers, Gaussians: complete ready to produce S2 result before the LSC meeting

S.Klimenko, February 2004, cit ligo seminar Summary l WaveBurst -low false alarm burst detection by using  Wavelet transform with low spectral leakage  TF coincidence at pixel level  Non-parametric statistics  Combined triple event confidence  Efficient VETO analysis l at the same time maintaining high detection efficiency