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.

Slides:



Advertisements
Similar presentations
Statistic for Combination of Results from Multiple Gravitational-Wave Searches Chris Pankow and Sergey Klimenko GWPAW 2011 Milwaukee, Wisconsin LIGO G v5G v5.
Advertisements

GWDAW-8 (December 17-20, 2003, Milwaukee, Wisconsin, USA) Search for burst gravitational waves with TAMA data Masaki Ando Department of Physics, University.
G.A.Prodi - INFN and Università di Trento, Italy International Gravitational Event Collaboration igec.lnl.infn.it ALLEGRO group:ALLEGRO (LSU)
Searching for pulsars using the Hough transform Badri Krishnan AEI, Golm (for the pulsar group) LSC meeting, Hanford November 2003 LIGO-G Z.
LIGO-G Z Coherent Coincident Analysis of LIGO Burst Candidates Laura Cadonati Massachusetts Institute of Technology LIGO Scientific Collaboration.
Systematic effects in gravitational-wave data analysis
The “probability event horizon” and probing the astrophysical GW background School of Physics University of Western Australia Research is funded by the.
G Z April 2007 APS Meeting - DAP GGR Gravitational Wave AstronomyKeith Thorne Coincidence-based LIGO GW Burst Searches and Astrophysical Interpretation.
Results from TOBAs Results from TOBAs Cross correlation analysis to search for a Stochastic Gravitational Wave Background University of Tokyo Ayaka Shoda.
DelayRatio: A Gravitational Wave Event Physical Likelihood Estimator Based on Detection Delays and SNR Ratios Amber L. Stuver LIGO Livingston ObservatoryCalifornia.
Soma Mukherjee GWDAW8, Milwaukee, Dec '03 Interferometric Data Modeling: Issues in realistic data generation. Soma Mukherjee CGWA University of Texas.
Data Characterization in Gravitational Waves Soma Mukherjee Max Planck Institut fuer Gravitationsphysik Golm, Germany. Talk at University of Texas, Brownsville.
Adapting matched filtering searches for compact binary inspirals in LSC detector data. Chad Hanna – For the LIGO Scientific Collaboration.
The Role of Data Quality in S5 Burst Analyses Lindy Blackburn 1 for the LIGO Scientific Collaboration 1 Massachusetts Institute of Technology, Cambridge,
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 M GWDAW, December LIGO Burst Search Analysis Laura Cadonati, Erik Katsavounidis LIGO-MIT.
Data Quality Vetoes in LIGO S5 Searches for Gravitational Wave Transients Laura Cadonati (MIT) For the LIGO Scientific Collaboration LIGO-G Z.
M. Principe, GWDAW-10, 16th December 2005, Brownsville, Texas Modeling the Performance of Networks of Gravitational-Wave Detectors in Bursts Search Maria.
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.
GRBs & VIRGO C7 run Alessandra Corsi & E. Cuoco, F. Ricci.
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,
ILIAS WP1 – Cascina IGEC – First experience using the data of 5 bar detectors: ALLEGRO, AURIGA, EXPLORER NAUTILUS and NIOBE. – 1460.
Searching for Gravitational Waves with LIGO Andrés C. Rodríguez Louisiana State University on behalf of the LIGO Scientific Collaboration SACNAS
S.Klimenko, August 2005, LSC, G Z Constraint likelihood analysis with a network of GW detectors S.Klimenko University of Florida, in collaboration.
LIGO-G D Status of Stochastic Search with LIGO Vuk Mandic on behalf of LIGO Scientific Collaboration Caltech GWDAW-10, 12/15/05.
Veto Selection for Gravitational Wave Event Searches Erik Katsavounidis 1 and Peter Shawhan 2 1 Massachusetts Institute of Technology, Cambridge, MA 02139,
Dec 16, 2005GWDAW-10, Brownsville Population Study of Gamma Ray Bursts S. D. Mohanty The University of Texas at Brownsville.
LIGO- G Z Analyzing Event Data Lee Samuel Finn Penn State University Reference: T030017, T
Gamma ray burst triggered searches in the S2, S3, S4 runs of LIGO Soumya D. Mohanty On behalf of the LIGO Science Collaboration.
Searching for Gravitational Waves from Binary Inspirals with LIGO Duncan Brown University of Wisconsin-Milwaukee for the LIGO Scientific 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.
A Data/Detector Characterization Pipeline (What is it and why we need one) Soumya D. Mohanty AEI January 18, 2001 Outline of the talk Functions of a Pipeline.
LIGO- G D Experimental Upper Limit from LIGO on the Gravitational Waves from GRB Stan Whitcomb For the LIGO Scientific Collaboration Informal.
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.
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.
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.
S.Klimenko, December 2003, GWDAW Burst detection method in wavelet domain (WaveBurst) S.Klimenko, G.Mitselmakher University of Florida l Wavelets l Time-Frequency.
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.
Comparison of filters for burst detection M.-A. Bizouard on behalf of the LAL-Orsay group GWDAW 7 th IIAS-Kyoto 2002/12/19.
Validation of realistically simulated non-stationary data. Soma Mukherjee Centre for Gravitational Wave Astronomy University of Texas at Brownsville. GWDAW9,
GWDAW11 – Potsdam Results by the IGEC2 collaboration on 2005 data Gabriele Vedovato for the IGEC2 collaboration.
Soma Mukherjee GWDAW8, Milwaukee, December'03 Interferometric Data Modeling: Issues in realistic data generation. Soma Mukherjee CGWA Dept. of Physics.
LIGO-G Z 23 October 2002LIGO Laboratory NSF Review1 Searching for Gravitational Wave Bursts: An Overview Sam Finn, Erik Katsavounidis and Peter.
The first AURIGA-TAMA joint analysis proposal BAGGIO Lucio ICRR, University of Tokyo A Memorandum of Understanding between the AURIGA experiment and the.
Searching the LIGO data for coincidences with Gamma Ray Bursts Alexander Dietz Louisiana State University for the LIGO Scientific Collaboration LIGO-G Z.
SEARCH FOR INSPIRALING BINARIES S. V. Dhurandhar IUCAA Pune, India.
LIGO-G Z Results from LIGO Observations Stephen Fairhurst University of Wisconsin - Milwaukee on behalf of the LIGO Scientific Collaboration.
Search for gravitational waves from binary inspirals in S3 and S4 LIGO data. Thomas Cokelaer on behalf of the LIGO Scientific Collaboration.
Search for compact binary systems in LIGO data Thomas Cokelaer On behalf of the LIGO Scientific Collaboration Cardiff University, U.K. LIGO-G Z.
Search for compact binary systems in LIGO data Craig Robinson On behalf of the LIGO Scientific Collaboration Cardiff University, U.K. LIGO-G
Thomas Cokelaer for the LIGO Scientific Collaboration Cardiff University, U.K. APS April Meeting, Jacksonville, FL 16 April 2007, LIGO-G Z Search.
Brennan Hughey MIT Kavli Institute Postdoc Symposium
A 2 veto for Continuous Wave Searches
Searching for pulsars using the Hough transform
The Q Pipeline search for gravitational-wave bursts with LIGO
Soma Mukherjee Centre for Gravitational Wave Astronomy
Results from TOBAs Cross correlation analysis to search for a Stochastic Gravitational Wave Background University of Tokyo Ayaka Shoda M. Ando, K. Okada,
M.-A. Bizouard, F. Cavalier
Maria Principe University of Sannio, Benevento, Italy
SLOPE: A MATLAB Revival
Search for gravitational waves from binary black hole mergers:
Coherent Coincident Analysis of LIGO Burst Candidates
Status and Plans for the LIGO-TAMA Joint Data Analysis
loosely modeled “burst” searches
Presentation transcript:

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 Confidence in Detection Upper Limits Detector Characterization

18/01/01GEO data analysis meeting, Golm Transient Tests Several Tests have been developed. –No uniformly most powerful transient detector known. –Need detectors that can exploit NR waveform information. Thorough comparison required. –One such project is already underway. (SDM, Patrice Hello, Eric Chassande-Motin.) Criteria for comparison –Receiver Operating Characteristics (ROC). –Robustness against noise models. –Robustness against signal models. –Computational requirements.

18/01/01GEO data analysis meeting, Golm Establishing Confidence in Detection Confidence: –Probability of detected event being not due to noise. –1 - (False alarm probability). What should be our level of confidence? False alarms: Terrestrial burst interference, instrumental noise. Primary means of establishing confidence –Coincidence between GW interferometers. –Coincidence between GW and Astronomical observations. –Anti-coincidence with auxiliary channels.

18/01/01GEO data analysis meeting, Golm Coincidence: GW detectors (I) False alarm rate (noise) in pairwise coincidence = r 1 r 2 w. r 1, r 2 = false alarm rates in each detector. w = window size. Detection probability = Q 1 Q 2 p. –Important: p comes from time of arrival estimation error. (It is also direction dependent.) –Estimation errors are threshold independent. For given SNR, Detection probability <= p. –p can become small if w is not sufficiently greater than.

18/01/01GEO data analysis meeting, Golm Coincidence: GW Detectors (II) For transients, time of arrival estimates will not be as good as for known waveform signals. –Will not be a surprise if the error is comparable to light travel time. Need a good estimate of the time of arrival estimate error variance. –Monte Carlo simulations required for complicated tests. –Detector characteristics used in simulations change with time.

18/01/01GEO data analysis meeting, Golm Coincidence: GW Detectors (III) How does SNR in coincidence scale with number of detectors ? –Coincidence cannot beat (Number of detectors) ½ scaling of SNR in Likelihood Ratio tests. Coincidences possible in other parameters –Each extra coincidence parameter means reduction in detection probability. –Note: As before, there will be a threshold independent limit on detection probability. –Estimation error covariance matrix required for correct window volume.

18/01/01GEO data analysis meeting, Golm Bar detectors Strategy: Detect an excess in coincidences. –Considerable experience available. –Do some of the same concerns apply? Other issues –Differing detector characteristics (e.g., noise PSD). –Cross-correlation based methods: Have to rule out terrestrial sources of cross-correlation, SNR goes as N ¼. Coincidence: GW Detectors (IV)

18/01/01GEO data analysis meeting, Golm Coincidence: GW with Astro. (I) Coincidence window in time for GW and Astro. event will not be known in general. –Method under development by Soma Mukherjee and SDM that makes window size a parameter that can be searched over for the best fit to the observed rates. –Can be generalized to include positional information. Positional coincidence: Too big an error box is a problem for counterpart searches. –Could do something like ROTSE or LOTIS: Fast, wide- field optical searches by robotic telescopes. –What is the confidence level required by astronomers? –Even if a candidate is found, may need to estimate GW burst waveform to form a plausible link.

18/01/01GEO data analysis meeting, Golm Coincidence: GW and Astro. (II) Use astronomical triggers to look for GW bursts. –Reduces data duration for search and, hence, false alarm rate (increases confidence). –Analysis for Binary Inspirals by Piran (1993). Need to put a selection on triggers. –Example: Most GRBs occur at large distances. Putting a distance cutoff can enhance confidence. Statistical Detection possible. –Finn, Mohanty, Romano, –Use triggers to “chop” between background and source and check for statistical difference. –Useful quantities can be calculated such as average GW burst strength.

18/01/01GEO data analysis meeting, Golm Anti-coincidence with Aux. Channels (I) Simple analysis. –For N aux. channels per site with false alarm rate of r in each channel, probability of at least one false anti-coincidence = 2 N r w. (w is the time window). –w = 2 sec, N = 10, r = 5/hour gives 1 out of 18 GW bursts falsely dismissed. False alarm rate for aux. channels may have large error –Example: actual r could be 10/hour: 1 per 10 GW bursts lost. –Robust test: false alarm rate independent of noise models (SDM, 2000). –This could also be an issue for GW-GW coincidence since false alarm rate r 1 r 2 w goes as square of individual false alarm rate.

18/01/01GEO data analysis meeting, Golm Robust Transient Test SDM, PRD, False alarm rate is independent of noise model. Made possible by –Adopting the weakest possible criterion for a transient: Brief episode of non-stationarity. No mention of Gaussianity or non-Gaussianity here. –Check for a change in the (only) measure of (wide sense) stationarity which is the PSD. Surprisingly good performance. –Can be improved by reducing robustness (= less general criterion for a transient).

18/01/01GEO data analysis meeting, Golm Anti-coincidence with Aux. Channels (II) Clearly, a simple anti-coincidence is not enough Need to establish if an aux. channel event could have caused the GW channel transient. –May require an end-to-end simulation software as being developed in the LIGO project. –Waveform estimation tools required. –Estimation also occurs in designing a proper GW-GW coincidence scheme (eg.,time of arrival estimation error). –Estimation seems to be intimately intertwined with detection.

18/01/01GEO data analysis meeting, Golm Upper Limits Upper limit on what? –Rate at a certain SNR, in some Bandwidth, in a certain class of bursts. –Max. SNR in a certain class of bursts. –Other quantities of Astrophysical interests. –Each quantity above requires its own analysis scheme. Combining upper limits on rates with coincidence analyses. –Much to learn from the Bar detector community. Important to characterize background (rate, distribution of amplitude etc.) –One possible way: Treat all non-coincident events as part of background. Estimate rate etc., from these events.

18/01/01GEO data analysis meeting, Golm Detector Characterization Instantaneous Detector “state” required –For estimating estimation errors and performance of transient tests via simulations. –Need to study estimation tools and fix what information constitutes detector state. Characterization of rate and amplitude distribution of terrestrial bursts required for upper limit calculations. –This requires keeping track of detector history. –Analyze almost all data: Need an automated pipeline!