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Gravitational-wave transient detection and multi-messenger - PowerPoint PPT Presentation

Gravitational-wave transient detection and multi-messenger astrophysics astrophysics Ray Frey, University of Oregon y y, y g for the LIGO Scientific Collaboration GO Sc e t c Co abo at o and the Virgo Collaboration LIGO-G1000515 LIGO


  1. Gravitational-wave transient detection and multi-messenger astrophysics astrophysics Ray Frey, University of Oregon y y, y g for the LIGO Scientific Collaboration GO Sc e t c Co abo at o and the Virgo Collaboration LIGO-G1000515 LIGO G1000515 • Introduction – overview and status of LIGO and Virgo • Observational results • A new astronomy with advanced GW detectors y G1000515 19July2010 TeVpa, Paris 1

  2. Required GW Sensitivity for Detection • GW emission requires time varying quadrupole moment of mass distribution quadrupole moment of mass distribution, → gravitational-wave strain, h = δ L/ L, is the analog of the radiation field E in E&M • Strain estimate: G1000515 19July2010 TeVpa, Paris 2

  3. GW Interferometer principle • Michelson interferometer with Fabry-Perot cavity arms. Long baseline: 4 km ( h = δ L/ L ) - For h ≈ 10 -21 , L ≈ 1 km, then δ L ≈ 10 -18 m Long baseline: 4 km ( h δ L/ L ) For h 10 • , L 1 km, then δ L 10 m Fabry-Perot Cavity storage time ∼ 1 ms ( ∼ 100 bounces) • • Power recycling (x30) • Noise estimate: 5 W 10 kW G1000515 19July2010 TeVpa, Paris 3

  4. Global network of interferometers LIGO GEO 600m VIRGO 3 km TAMA 300m TAMA 300m 4 km & 2 km 4 km & 2 km → LCGT ! → LCGT ! LSC: LIGO+GEO AIGO- R&D LIGO LIGO 4 km → “LIGO A Australia” ? t li ” ? G1000515 19July2010 TeVpa, Paris 4

  5. S5/VSR1 sensitivity 2007 LIGO Run S5: 2005-07 Ran at design sensitivity for initial LIGO Virgo Run VSR1: 2007 Data sharing with g LIGO/GEO LIGO S5 S6 Adv LIGO 2006 2007 2008 2009 2010 2011 2012 2013 2014 2015 Virgo VS R1 R3 R2 Adv Virgo G1000515 19July2010 TeVpa, Paris 5

  6. The LIGO-Virgo network: sky coverage aver LIGO O Hanford rage antenna factor h(t) = F h (t) + F h (t) h(t) F x h x (t) + F + h + (t) F + ⊕ F x F + ⊕ F x ave Virg erage anten go nna factor + GRBs in S5/VSR1 G1000515 19July2010 TeVpa, Paris 6

  7. GW signals classification Short duration Long duration un- modeled Burst search Stochastic search matched matched Inspiral search Inspiral search CW search CW search filter Credit: NASA/CXC/ASU/J. Hester et al. G1000515 19July2010 TeVpa, Paris 7

  8. S5/VSR1 sensitivity to compact binary coalescence p y • NS-NS, NS-BH, BH-BH • Efficient GW radiators: ~10 -2 Mc 2 • Matched filter analysis for low-mass inspirals (horizon= (horizon= distance to optimally oriented and located binary which gives SNR=8 in one detector) G1000515 19July2010 TeVpa, Paris 8

  9. S5/VSR1 sensitivity to GW Bursts • short (< 1s) transients • unmodeled waveforms • CCSNe, GRBs, SGRs, … t (ms) π 2 3 c ≈ 2 2 2 E D f f h GW GW 0 0 rss rss G G G1000515 19July2010 TeVpa, Paris 9

  10. LIGO-Virgo Search Results • No GW detections yet • H However, beginning to make astrophysically interesting limits b i i t k t h i ll i t ti li it � This talk: Astrophysically targeted transient searches (GRBs, SGRs) � Others: Others: • Crab pulsar spindown limit (ApJ 683 (2008) 45 ) • cosmic GW background limit < BBN (Nature 460 (2009) 990 ) • Era of advanced GW detectors is approaching (>2014) in which we Era of advanced GW detectors is approaching (>2014) in which we expect GW detections will become frequent (more on this later) • To take advantage of this opportunity, we have developed a suite of multi-messenger pathways to fully explore the science (this talk) th t f ll l th i (thi t lk) lti G1000515 19July2010 TeVpa, Paris 10

  11. Multi-messenger astronomy with GWs EM EM , neutrinos neutrinos External Follow Triggers Triggers Ups Ups GW G1000515 19July2010 TeVpa, Paris 11

  12. Multi-messenger astronomy with GWs • Detection confidence • Event time • Sky position • • Improved search sensitivity Improved search sensitivity • Redshift • Progenitor information g G1000515 19July2010 TeVpa, Paris 12

  13. Multi-messenger astronomy with GWs – Status • Externally triggered searches – gamma, X-rays (Swift, Fermi, IPN) � GRBs GRB � SGRs • Externally triggered searches – neutrinos Externally triggered searches neutrinos � High-energy neutrinos (Ice Cube, ANTARES , …) • GRBs, ? � Low-energy neutrinos (Super-K, LVD, Borexino,…) • Core-collapse supernovae • • Electromagnetic follow ups of GW triggers Electromagnetic follow-ups of GW triggers � Requires fast (~10 min) id and distribution of LIGO-Virgo trigger (for S6) • ~few degree resolution with LIGO-Virgo network � Swift ToO – XRT � Wide-angle optical telescopes (SkyMapper, TAROT, Quest, …) � Radio � Radio G1000515 19July2010 TeVpa, Paris 13

  14. Multi-messenger astronomy with GWs – Status • Externally triggered searches – gamma, X-rays (Swift, Fermi, IPN) � GRBs GRB Past and ongoing � SGRs searches • Externally triggered searches – neutrinos Externally triggered searches neutrinos � High-energy neutrinos (Ice Cube, Antares, …) • GRBs, ? � Low-energy neutrinos (Super-K, LVD, Borexino,…) • Core-collapse supernovae • • Electromagnetic follow ups of GW triggers Electromagnetic follow-ups of GW triggers � Requires fast (~10 min) id and distribution of LIGO-Virgo trigger (for S6) • ~few degree resolution with LIGO-Virgo network � Swift ToO – XRT � Wide-angle optical telescopes (SkyMapper, TAROT, Quest, … ) � Radio � Radio G1000515 19July2010 TeVpa, Paris 14

  15. Gamma-ray Bursts and GWs Long duration GRBs Long-duration GRBs BATSE BATSE • Associated with core-collapse of massive stars (“hypernovae”) GSFC Both progenitor models would also give GW emission also give GW emission Short-duration GRBs • Mergers are efficient GW radiators • Associated with binary mergers ~ 10 -2 Mc 2 E GW ~ 10 E Mc (NS NS NS BH) (NS-NS, NS-BH) • Massive core collapse – unknown, but expected to be less efficient G1000515 19July2010 TeVpa, Paris 15

  16. GRB 070201 • GRB 070201 – a short-duration gamma ray burst with position gamma-ray burst with position consistent with M31 (Andromeda), 0.8 Mpc away. • Such a nearby GRB would have easily been observed by LIGO if due easily been observed by LIGO if due to a binary merger • This hypothesis ruled out at ~99% CL Revised error box • • Most likely: SGR in M31 (E iso ~10 45 Most likely: SGR in M31 (E ~10 45 M Mazets et al., ApJ 680, 545 l A J 680 4 erg) • Astrophys. J. 681 (2008) 1419 G1000515 19July2010 TeVpa, Paris 16

  17. GRB 070201 (contd) Binary coalescence exclusion: Also searched for unmodeled bursts: Unable to exclude SGR from M31 G1000515 19July2010 TeVpa, Paris 17

  18. Search for GWs from SGRs • Soft Gamma Repeaters are thought to be magnetars – highly magnetized neutron stars Can emit occasional EM flares (~10 42 erg), • giant flares (~10 46 erg), or flare “storms” • Flare mechanism (crust cracking) would Flare mechanism (crust cracking) would excite vibrational modes → GWs General idea: Look for GW in coincidence with flares + flare ◊ giant flare ∗ storm G1000515 19July2010 TeVpa, Paris 18

  19. SGRs (contd) • Search for long-lived quasiperiodic GWs after giant flare SGR 1806-20 � GW energy limits are comparable to total EM energy emission PRD 76 (2007) 062003 (LSC) � • Search for GW bursts at times of 190 flares from 1806-20, 1900+14 � Excess power search for neutron star f -modes (~1.5–3 kHz) and arbitrary lower-frequency bursts � GW energy limits as low as few × 10 45 erg; PRL 101 (2008) 21110 GW energy limits as low as few × 10 erg; PRL 101 (2008) 21110 • Stack GW signal power from each flare in 2006 SGR 1900+14 “storm”: Swift, SGR1900+14 storm 30 s 0 � GW energy limit few × 10 45 erg; ApJ 701 (2009) L68 . 10 45 GW li i f A J 01 (2009) L68 G1000515 19July2010 TeVpa, Paris 19

  20. Advanced GW detectors LIGO S5 S6 GEO HF Adv LIGO 2006 2007 2008 2009 2010 2011 2012 2013 2014 2015 Virgo VS R1 Virgo VS R1 R3 R3 R2 R2 Adv Virgo Adv Virgo Install Advanced LIGO Advanced LIGO and Virgo • Major upgrades � � Lasers, optics, suspensions Lasers optics suspensions � Limited by Quantum noise • 10x better sensitivity • 1000x bigger search volume Some elements of advanced Some elements of advanced detectors implemented already in S6 and VSR3 G1000515 19July2010 TeVpa, Paris 20

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