1 / 15

Waveforms for Binary Black Holes - Late Stages of In-spiral and Merger

Waveforms for Binary Black Holes - Late Stages of In-spiral and Merger. B.S. Sathyaprakash LIGO-G010153-00-Z. Plan of the talk. Prospects for detecting binaries in initial interferometers Re-summed approach to GW phasing

brie
Télécharger la présentation

Waveforms for Binary Black Holes - Late Stages of In-spiral and Merger

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Waveforms for Binary Black Holes - Late Stages of In-spiral and Merger B.S. Sathyaprakash LIGO-G010153-00-Z LSC@Baton Rouge

  2. Plan of the talk • Prospects for detecting binaries in initial interferometers • Re-summed approach to GW phasing • P-approximants - taming poorly convergent post-Newtonian expansion - Kerr case • Effective one-body - inspiral + plunge • Improvement in SNR by including plunge • Search strategy LSC@Baton Rouge

  3. Sensitivity of first interferometers LSC@Baton Rouge

  4. Signal-to-noise ratios for inspiralDamour, Iyer, Sathyaprakash 2000 LSC@Baton Rouge

  5. Why bother using non-post-Newtonian waveformsDIS 98, 00; BD 98, 00; DJS 99; D 01 • Standard post-Newtonian expansion is very slowly convergent • Re-summation techniques are proven to be convergent and robust in the test mass limit • There are no alternatives to deal with physics close to, and beyond, the last stable orbit LSC@Baton Rouge

  6. Exact GW flux - Kerr Case Tanaka 96 a=0.0, 0.25, 0.5, 0.75, 0.95 LSC@Baton Rouge

  7. Post-Newtonian flux - Kerr caseTanaka et al 96 a=0.0, 0.25, 0.5, 0.75, 0.95 LSC@Baton Rouge

  8. P-approximant flux - Kerr casePorter 01 a=0.0, 0.25, 0.5, 0.75, 0.95 LSC@Baton Rouge

  9. Probing inspiral, plunge and merger LSC@Baton Rouge

  10. Effective one-body approach Buonanno and Damour 98, 00 • Condense essential information about the dynamics in just one function - a radial potential: A(r=M/u) = 1-2u+2h u3 +a4(h,ws)u4 + … • The unknown coefficient ws, at 3PN level does not affect the overlaps severely • Allows the computation of the orbit beyond the last stable orbit up to r ~ 2.8M plunge LSC@Baton Rouge

  11. EOB waveformBuonanno and Damour 00 LSC@Baton Rouge

  12. EOB signal in frequency domainDamour, Iyer and Sathyaprakash 00 EOB Signals are wide-band LSC@Baton Rouge

  13. Improvement in SNR while using EOB signalsDamour, Iyer and Sathyaprakash 01 LSC@Baton Rouge

  14. Relative performance of different approximantsDamour, Iyer and Sathyaprakash 01 LSC@Baton Rouge

  15. What waveforms should we use in our search codes? • LIGO-GEO network gives us a unique opportunity to make reliable detection of unreliable signals (4-way coincidence) • Low mass region, SPA or P-approximants • Our best candidates are BH-BH binaries • Binaries with 10-40 solar masses, number of templates required is about 10; employ EOB waveforms and expand search space around this family LSC@Baton Rouge

More Related