S.Klimenko, December 2003, GWDAW Burst detection method in wavelet domain (WaveBurst) S.Klimenko, G.Mitselmakher University of Florida l Wavelets l Time-Frequency.

Slides:



Advertisements
Similar presentations
Applications in Signal and Image Processing
Advertisements

Extensions of wavelets
GWDAW-8 (December 17-20, 2003, Milwaukee, Wisconsin, USA) Search for burst gravitational waves with TAMA data Masaki Ando Department of Physics, University.
Comparing different searches for gravitational-wave bursts on simulated LIGO and VIRGO data Michele Zanolin -MIT on behalf of the LIGO-VIRGO joint working.
E12 Report from the Burst Group Burst Analysis Group and the Glitch Investigation Team.
Descriptive statistics Experiment  Data  Sample Statistics Experiment  Data  Sample Statistics Sample mean Sample mean Sample variance Sample variance.
S.Klimenko, February 2004, cit ligo seminar Excess power method in wavelet domain for burst searches (WaveBurst) S.Klimenko University of Florida l Introduction.
Introduction To Signal Processing & Data Analysis
LIGO-G Z Coherent Coincident Analysis of LIGO Burst Candidates Laura Cadonati Massachusetts Institute of Technology LIGO Scientific Collaboration.
Wavelets: theory and applications
Spinning Black Hole Binaries1 Search for Spinning Black Hole Binaries in Advanced LIGO: Parameter tuning of HACR Speaker: Gareth Jones Cardiff University.
G Z April 2007 APS Meeting - DAP GGR Gravitational Wave AstronomyKeith Thorne Coincidence-based LIGO GW Burst Searches and Astrophysical Interpretation.
Waveburst DSO: current state, testing on S2 hardware burst injections Sergei Klimenko Igor Yakushin LSC meeting, March 2003 LIGO-G Z.
UF S.Klimenko LIGO-G Z l Introduction l Goals of this analysis l Coherence of power monitors l Sign X-Correlation l H2-L1 x-correlation l Conclusion.
Results from TOBAs Results from TOBAs Cross correlation analysis to search for a Stochastic Gravitational Wave Background University of Tokyo Ayaka Shoda.
LIGO-G Z Detector characterization for LIGO burst searches Shourov K. Chatterji for the LIGO Scientific Collaboration 10 th Gravitational Wave.
New data analysis for AURIGA Lucio Baggio Italy, INFN and University of Trento AURIGA.
Observing the Bursting Universe with LIGO: Status and Prospects Erik Katsavounidis LSC Burst Working Group 8 th GWDAW - UWM Dec 17-20, 2003.
S.Klimenko, G Z, December 21, 2006, GWDAW11 Coherent detection and reconstruction of burst events in S5 data S.Klimenko, University of Florida.
A coherent null stream consistency test for gravitational wave bursts Antony Searle (ANU) in collaboration with Shourov Chatterji, Albert Lazzarini, Leo.
LIGO-G Z Peter Shawhan, for the LIGO Scientific Collaboration APS Meeting April 25, 2006 Search for Gravitational Wave Bursts in Data from the.
LIGO-G M GWDAW, December LIGO Burst Search Analysis Laura Cadonati, Erik Katsavounidis LIGO-MIT.
School of Biomedical Engineering, Science and Health Systems APPLICATION OF WAVELET BASED FUSION TECHNIQUES TO PHYSIOLOGICAL MONITORING Han C. Ryoo, Leonid.
LIGO-G Z Coherent Analysis of Signals from Misaligned Interferometers M. Rakhmanov, S. Klimenko Department of Physics, University of Florida,
LIGO-G Z 1 Data analysis for impulsive signals using interferometers Peter R. Saulson Syracuse University Spokesperson, LIGO Scientific Collaboration.
The Analysis of Binary Inspiral Signals in LIGO Data Jun-Qi Guo Sept.25, 2007 Department of Physics and Astronomy The University of Mississippi LIGO Scientific.
S.Klimenko, December 2003, GWDAW Performance of the WaveBurst algorithm on LIGO S2 playground data S.Klimenko (UF), I.Yakushin (LLO), G.Mitselmakher (UF),
Searching for Gravitational Waves with LIGO Andrés C. Rodríguez Louisiana State University on behalf of the LIGO Scientific Collaboration SACNAS
S.Klimenko, July 14, 2007, Amaldi7,Sydney, G Z Detection and reconstruction of burst signals with networks of gravitational wave detectors S.Klimenko,
18/01/01GEO data analysis meeting, Golm Issues in GW bursts Detection Soumya D. Mohanty AEI Outline of the talk Transient Tests (Transient=Burst) Establishing.
Amaldi-7 meeting, Sydney, Australia, July 8-14, 2007 LIGO-G Z All-Sky Search for Gravitational Wave Bursts during the fifth LSC Science Run Igor.
Yousuke Itoh GWDAW8 UW Milwaukee USA December 2003 A large value of the detection statistic indicates a candidate signal at the frequency and.
Dec 16, 2005GWDAW-10, Brownsville Population Study of Gamma Ray Bursts S. D. Mohanty The University of Texas at Brownsville.
G030XXX-00-Z Excess power trigger generator Patrick Brady and Saikat Ray-Majumder University of Wisconsin-Milwaukee LIGO Scientific Collaboration.
Searching for Gravitational Waves from Binary Inspirals with LIGO Duncan Brown University of Wisconsin-Milwaukee for the LIGO Scientific Collaboration.
S.Klimenko, August 2003, Hannover LIGO-G Z How optimal are wavelet TF methods? S.Klimenko l Introduction l Time-Frequency analysis l Comparison.
1 Laura Cadonati, MIT For the LIGO Scientific Collaboration APS meeting Tampa, FL April 16, 2005 LIGO Hanford ObservatoryLIGO Livingston Observatory New.
LIGO-G Z The Q Pipeline search for gravitational-wave bursts with LIGO Shourov K. Chatterji for the LIGO Scientific Collaboration APS Meeting.
S.Klimenko, G Z, December 2006, GWDAW11 Coherent detection and reconstruction of burst events in S5 data S.Klimenko, University of Florida for.
This material is based upon work supported in part by National Science Foundation Award PHY May 30-31, 2003, LIGO G Z APS NW Section Meeting.
S.Klimenko, G Z, December 21, 2006, GWDAW11 Coherent detection and reconstruction of burst events in S5 data S.Klimenko, University of Florida.
S.Klimenko, LSC, August 2004, G Z BurstMon S.Klimenko, A.Sazonov University of Florida l motivation & documentation l description & results l.
S.Klimenko, G Z, March 20, 2006, LSC meeting First results from the likelihood pipeline S.Klimenko (UF), I.Yakushin (LLO), A.Mercer (UF),G.Mitselmakher.
The 9th Gravitational Wave Data Analysis Workshop (December 15-18, 2004, Annecy, France) Results of the search for burst gravitational waves with the TAMA300.
LIGO-G Z Confidence Test for Waveform Consistency of LIGO Burst Candidate Events Laura Cadonati LIGO Laboratory Massachusetts Institute of Technology.
Data Analysis Algorithm for GRB triggered Burst Search Soumya D. Mohanty Center for Gravitational Wave Astronomy University of Texas at Brownsville On.
S.Klimenko, March 2003, LSC Burst Analysis in Wavelet Domain for multiple interferometers LIGO-G Z Sergey Klimenko University of Florida l Analysis.
LIGO-G Z GWDAW9 December 17, Search for Gravitational Wave Bursts in LIGO Science Run 2 Data John G. Zweizig LIGO / Caltech for the LIGO.
Peter Shawhan The University of Maryland & The LIGO Scientific Collaboration Penn State CGWP Seminar March 27, 2007 LIGO-G Z Reaching for Gravitational.
LIGO-G Z TFClusters Tuning for the LIGO-TAMA Search Patrick Sutton LIGO-Caltech.
S.Klimenko, LSC, Marcht 2005, G Z BurstMon diagnostic of detector noise during S4 run S.Klimenko University of Florida l burstMon FOMs l S4 run.
Igor Yakushin, December 2004, GWDAW-9 LIGO-G Z Status of the untriggered burst search in S3 LIGO data Igor Yakushin (LIGO Livingston Observatory)
S.Klimenko, LSC meeting, March 2002 LineMonitor Sergey Klimenko University of Florida Other contributors: E.Daw (LSU), A.Sazonov(UF), J.Zweizig (Caltech)
The first AURIGA-TAMA joint analysis proposal BAGGIO Lucio ICRR, University of Tokyo A Memorandum of Understanding between the AURIGA experiment and the.
SEARCH FOR INSPIRALING BINARIES S. V. Dhurandhar IUCAA Pune, India.
LIGO-G Z The Q Pipeline search for gravitational-wave bursts with LIGO Shourov K. Chatterji for the LIGO Scientific Collaboration APS Meeting.
LIGO-G05????-00-Z Detector characterization for LIGO burst searches Shourov K. Chatterji For the LIGO Scientific Collaboration 10 th Gravitational Wave.
Bounding the strength of gravitational radiation from Sco-X1
The Q Pipeline search for gravitational-wave bursts with LIGO
LIGO Scientific Collaboration meeting
Bounding the strength of gravitational radiation from Sco-X1
Coherent detection and reconstruction
WaveMon and Burst FOMs WaveMon WaveMon FOMs Summary & plans
Travis Hansen, Marek Szczepanczyk, Michele Zanolin
WaveBurst upgrade for S3 analysis
Excess power trigger generator
Search for gravitational waves from binary black hole mergers:
Coherent Coincident Analysis of LIGO Burst Candidates
A Waveform Consistency Test for Binary Inspirals using LIGO data
Performance of the WaveBurst algorithm on LIGO S2 playground data
Presentation transcript:

S.Klimenko, December 2003, GWDAW Burst detection method in wavelet domain (WaveBurst) S.Klimenko, G.Mitselmakher University of Florida l Wavelets l Time-Frequency analysis l Coincidence l Statistical approach l Summary

S.Klimenko, December 2003, GWDAW 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, December 2003, GWDAW 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, December 2003, GWDAW 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, December 2003, GWDAW Choice of Wavelet Wavelet “time-scale” plane wavelet resolution: 64 Hz X 1/128 sec Symlet Daubechies Biorthogonal  =1 ms  =100 ms sg850Hz

S.Klimenko, December 2003, GWDAW burst 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  works for 2 and more interferometers  coincidence at pixel level applied before triggers are produced

S.Klimenko, December 2003, GWDAW “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, December 2003, GWDAW 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, December 2003, GWDAW 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, December 2003, GWDAW 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, December 2003, GWDAW 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, December 2003, GWDAW 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, December 2003, GWDAW 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, December 2003, GWDAW 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, December 2003, GWDAW Summary A wavelet time-frequency method for detection of un- modeled bursts of GW radiation is presented  Allows different scale resolutions and wide choice of template waveforms.  Uses non-parametric statistics  robust operation with non-gaussian detector noise  simple tuning, predictable false alarm rates  Works for multiple interferometers  TF coincidence at pixel level  low black pixel threshold