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

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Presentation on theme: "S.Klimenko, August 2005, LSC, G050434-00-Z Constraint likelihood analysis with a network of GW detectors S.Klimenko University of Florida, in collaboration."— Presentation transcript:

1 S.Klimenko, August 2005, LSC, G050434-00-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/0508068

2 S.Klimenko, August 2005, LSC, G050434-00-Z Likelihood analysis for bursts l Outlined at  Flanagan, Hughes, PRD57 4577 (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 -

3 S.Klimenko, August 2005, LSC, G050434-00-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

4 S.Klimenko, August 2005, LSC, G050434-00-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)

5 S.Klimenko, August 2005, LSC, G050434-00-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

6 S.Klimenko, August 2005, LSC, G050434-00-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

7 S.Klimenko, August 2005, LSC, G050434-00-Z Network sensitivity factor H1-L1 +GEO +VIRGO +TAMA need several detectors for more uniform sky coverage

8 S.Klimenko, August 2005, LSC, G050434-00-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-G050361-00-Z)

9 S.Klimenko, August 2005, LSC, G050434-00-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

10 S.Klimenko, August 2005, LSC, G050434-00-Z Comparison of different methods Source at  =120,  =80, SNR~13 H1-L1-GEO hard soft standard

11 S.Klimenko, August 2005, LSC, G050434-00-Z ROC H1 L1 GEO =5 =8 sources uniformly distributed over the sky sky average SNR = 7 H1-L1-GEO

12 S.Klimenko, August 2005, LSC, G050434-00-Z Angular resolution for different methods fraction of events in the cone |detected-injected|<16 degrees H1 L1 GEO

13 S.Klimenko, August 2005, LSC, G050434-00-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

14 S.Klimenko, August 2005, LSC, G050434-00-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

15 S.Klimenko, August 2005, LSC, G050434-00-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)


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