S.Klimenko, August 2005, LSC, G050434-00-Z Constraint likelihood analysis with a network of GW detectors S.Klimenko University of Florida, in collaboration.

Slides:



Advertisements
Similar presentations
| October 12, 2011 A Multiple Signal Classification Method for Directional Gravitational-wave Burst Search Junwei.
Advertisements

Bayesian burst detection Antony Searle (ANU) with Patrick Sutton (Cardiff / LIGO Caltech), Massimo Tinto (JPL / LIGO Caltech), Shourov Chatterji (INFN.
Coherent network searches for gravitational-wave bursts Patrick Sutton LIGO-Caltech.
LIGO-G Z Coherent Coincident Analysis of LIGO Burst Candidates Laura Cadonati Massachusetts Institute of Technology LIGO Scientific Collaboration.
G Z April 2007 APS Meeting - DAP GGR Gravitational Wave AstronomyKeith Thorne Coincidence-based LIGO GW Burst Searches and Astrophysical Interpretation.
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.
1/25 Current results and future scenarios for gravitational wave’s stochastic background G. Cella – INFN sez. Pisa.
S.Klimenko, G Z, December 21, 2006, GWDAW11 Coherent detection and reconstruction of burst events in S5 data S.Klimenko, University of Florida.
Search for gravitational-wave bursts associated with gamma-ray bursts using the LIGO detectors Soumya D. Mohanty On behalf of the LIGO Scientific Collaboration.
Mock Data Production, Characteristics, and Confusion Background WG4 f2f – Nice 09/01/10 Tania Regimbau.
Silvia Poggi - GW burst detection strategy in non-homogeneus networks Detection strategies for bursts in networks of non-homogeneus gravitational waves.
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 Z The AURIGA-LIGO Joint Burst Search L. Cadonati, G. Prodi, L. Baggio, S. Heng, W. Johnson, A. Mion, S. Poggi, A. Ortolan, F. Salemi, P.
LIGO-G Z Coherent Analysis of Signals from Misaligned Interferometers M. Rakhmanov, S. Klimenko Department of Physics, University of Florida,
LIGO-G Z A Coherent Network Burst Analysis Patrick Sutton on behalf of Shourov Chatterji, Albert Lazzarini, Antony Searle, Leo Stein, Massimo.
S.Klimenko, December 2003, GWDAW Performance of the WaveBurst algorithm on LIGO S2 playground data S.Klimenko (UF), I.Yakushin (LLO), G.Mitselmakher (UF),
Solution of the Inverse Problem for Gravitational Wave Bursts Massimo Tinto JPL/CIT LIGO Seminar, October 12, 2004 Y. Gursel & M. Tinto, Phys. Rev. D,
Searching for Gravitational Waves with LIGO Andrés C. Rodríguez Louisiana State University on behalf of the LIGO Scientific Collaboration SACNAS
LIGO-G Z April 2006 APS meeting Igor Yakushin (LLO, Caltech) Search for Gravitational Wave Bursts in LIGO’s S5 run Igor Yakushin (LLO, Caltech)
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.
A fully coherent analysis can be performed when data is available from three or more non-aligned detectors Generalization of collocated Hanford detector.
Dec 16, 2005GWDAW-10, Brownsville Population Study of Gamma Ray Bursts S. D. Mohanty The University of Texas at Brownsville.
LIGO-G Z Results of the LIGO-TAMA S2/DT8 Joint Bursts Search Patrick Sutton LIGO Laboratory, Caltech, for the LIGO-TAMA Joint Working Group.
A fully coherent analysis can be performed when data is available from three or more non-aligned detectors Generalization of collocated Hanford detector.
S.Klimenko, December 16, 2007, GWDAW12, Boston, LIGO-G Z Coherent burst searches for gravitational waves from compact binary objects S.Klimenko,
Gamma ray burst triggered searches in the S2, S3, S4 runs of LIGO Soumya D. Mohanty On behalf of the LIGO Science Collaboration.
1 Status of Search for Compact Binary Coalescences During LIGO’s Fifth Science Run Drew Keppel 1 for the LIGO Scientific Collaboration 1 California Institute.
S.Klimenko, August 2003, Hannover LIGO-G Z How optimal are wavelet TF methods? S.Klimenko l Introduction l Time-Frequency analysis l Comparison.
LIGO-G Data Analysis Techniques for LIGO Laura Cadonati, M.I.T. Trento, March 1-2, 2007.
1 Laura Cadonati, MIT For the LIGO Scientific Collaboration APS meeting Tampa, FL April 16, 2005 LIGO Hanford ObservatoryLIGO Livingston Observatory New.
T.Akutsu, M.Ando, N.Kanda, D.Tatsumi, S.Telada, S.Miyoki, M.Ohashi and TAMA collaboration GWDAW10 UTB Texas 2005 Dec. 13.
S.Klimenko, G Z, December 2006, GWDAW11 Coherent detection and reconstruction of burst events in S5 data S.Klimenko, University of Florida for.
S.Klimenko, G Z, December 21, 2006, GWDAW11 Coherent detection and reconstruction of burst events in S5 data S.Klimenko, University of Florida.
Joint LIGO-Virgo data analysis Inspiral and Burst Summary of the first project results Overview of the future activities M.-A. Bizouard (LAL-Orsay) on.
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.
Coherent network analysis technique for discriminating GW bursts from instrumental noise Patrick Sutton (CIT) in collaboration with Shourov Chatterji,
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.
LIGO-G All-Sky Burst Search in the First Year of the LSC S5 Run Laura Cadonati, UMass Amherst For the LIGO Scientific Collaboration GWDAW Meeting,
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 Status of the LIGO-TAMA Joint Bursts Search Patrick Sutton LIGO Laboratory, Caltech, for the LIGO-TAMA Joint Working Group.
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.
G Z The LIGO gravitational wave detector consists of two observatories »LIGO Hanford Observatory – 2 interferometers (4 km long arms and 2 km.
LIGO-G ZSearle LSC Mtg Aug A Coherent Network Burst Analysis Antony Searle (ANU) in collaboration with Shourov Chatterji, Albert Lazzarini,
Soma Mukherjee LSC, Hanford, Aug.19 '04 Generation of realistic data segments: production and application. Soma Mukherjee Centre for Gravitational Wave.
Igor Yakushin, December 2004, GWDAW-9 LIGO-G Z Status of the untriggered burst search in S3 LIGO data Igor Yakushin (LIGO Livingston Observatory)
LIGO-G Z Searching for gravitational wave bursts with the new global detector network Shourov K. Chatterji INFN Sezioni di Roma / Caltech LIGO.
LIGO-G Z Status of the LIGO-TAMA Joint Bursts Search Patrick Sutton LIGO Laboratory, Caltech, for the LIGO-TAMA Joint Working Group.
LIGO-G Z Results from LIGO Observations Stephen Fairhurst University of Wisconsin - Milwaukee on behalf of the LIGO Scientific Collaboration.
P.Astone, S.D’Antonio, S.Frasca, C.Palomba
Soma Mukherjee Centre for Gravitational Wave Astronomy
Igor Yakushin, LIGO Livingston Observatory
Searching for gravitational wave bursts with the new global detector network 2007 May 3 Searching for gravitational wave bursts with the new global detector.
Searching for Gravitational-Wave Bursts (GWBs) associated with Gamma-Ray Bursts (GRBs) during the LIGO S5 run Isabel Leonor University of Oregon (for the.
Coherent detection and reconstruction
WaveMon and Burst FOMs WaveMon WaveMon FOMs Summary & plans
M.-A. Bizouard, F. Cavalier
Targeted Searches using Q Pipeline
WaveBurst upgrade for S3 analysis
Status of the LIGO-TAMA Joint Data Analyses
Status and Plans for the LIGO-TAMA Joint Data Analysis
with coherent WaveBurst pipeline
Performance of the WaveBurst algorithm on LIGO S2 playground data
Presentation transcript:

S.Klimenko, August 2005, LSC, G Z Constraint likelihood analysis with a network of GW detectors S.Klimenko University of Florida, in collaboration with S.Mohanty,M.Rakhmanov,G.Mitselmakher l Likelihood analysis l Two detector paradox l Network sensitivity to GW polarizations l Constraint likelihood l Results & Summary gr-qc/

S.Klimenko, August 2005, LSC, G Z Likelihood analysis for bursts l Outlined at  Flanagan, Hughes, PRD (1998)  Mohanty et al, CQG 21 S1831 (2004) Likelihood for Gaussian noise with variance  2 k and GW waveform u: x k [i] – detector output, F k – antenna patterns l For unknown GW signal treat every sample of u as an independent variable  find u[i] from variation of L detector response -

S.Klimenko, August 2005, LSC, G Z Solution for GW waveforms l Given by two linear equations: l Network response matrix M R l Network data vector l Network antenna patterns l Solution: -- estimator of GW waveform Sum over detectors detection statistic is obtained from the likelihood functional by substituting u with the solution

S.Klimenko, August 2005, LSC, G Z Two detector paradox l aligned detectors (unit noise variance for simplicity):  If separated  L A has directional sensitivity (circle on the sky) l misaligned detectors (even infinitesimally):  solution for GW waveform: No directional sensitivity for two misaligned detectors! power cross-correlation (Johnston, Mohanty)

S.Klimenko, August 2005, LSC, G Z Dominant polarization wave frame l such a wave frame where the network antenna pattern g c is positive and real  g – network sensitivity factor   – network alignment factor l diagonal M R  independent statistics for h 1 & h 2 -- GW polarizations in the DP frame l total signal l Only first component is detected if -sum-square energies of GW polarizations

S.Klimenko, August 2005, LSC, G Z Network alignment factor shows relative sensitivity to two GW components For aligned network  =0 blue<0.1 H1-L1 +GEO +VIRGO +TAMA to be detected with the same SNR h 2 should be 1/  times stronger then h 1

S.Klimenko, August 2005, LSC, G Z Network sensitivity factor H1-L1 +GEO +VIRGO +TAMA need several detectors for more uniform sky coverage

S.Klimenko, August 2005, LSC, G Z constraint l In average for a population of bursts expect l Hard constraint  ignore the second component l Soft constraint  weight the second component  remove un-physical solutions produced by noise  sacrifice small fraction of GW signals but  enhance detection efficiency for the rest of sources another approach: penalized likelihood (Mohanty et al, LIGO-G Z)

S.Klimenko, August 2005, LSC, G Z Two detector sky maps Source at  =120  =80 Constraint likelihood gives directional information in the case of two detectors H1-L1 H1-G1 Simulation Equal detector sensitivity white, G-noise injections: -Lazarus BH-BH -2-polarizations

S.Klimenko, August 2005, LSC, G Z Comparison of different methods Source at  =120,  =80, SNR~13 H1-L1-GEO hard soft standard

S.Klimenko, August 2005, LSC, G Z ROC H1 L1 GEO =5 =8 sources uniformly distributed over the sky sky average SNR = 7 H1-L1-GEO

S.Klimenko, August 2005, LSC, G Z Angular resolution for different methods fraction of events in the cone |detected-injected|<16 degrees H1 L1 GEO

S.Klimenko, August 2005, LSC, G Z WaveBurst.net SG20 injections into S4 data Simulated LIGO noise H1-H2-L1 l WAT/DMT implementation (klimenko) l First run on S4 data with SG20 injections (Yakushin) Likelihood vs WaveBurst significance

S.Klimenko, August 2005, LSC, G Z Likelihood l Likelihood distribution of WaveBurst triggers for  Simulated LIGO noise (black)  SG20 injections into S4 data (blue, red) WB significance >1.9 No selection on WB significance

S.Klimenko, August 2005, LSC, G Z Summary l Coherent network method for GW bursts searches  Based on the likelihood analysis  Obtain max likelihood ratio statistics by constrained variation of likelihood functional  detection statistic uses both power and cross-correlation terms  give information about source location, waveform reconstruction  any number of detectors, arbitrary alignment l Plans  Finish debugging of hierarchical search WaveBurst.net  Study waveform and coordinate reconstruction on simulations  Compare with r-statistics for H1-H2-L1 (useful cross-check)  Analyze S 4 LIGO-GEO data  get ready for S5  Implement non-hierarchical search (cpu consuming)