T. Regimbau
Centre national de la recherche scientifique
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Featured researches published by T. Regimbau.
Physical Review X | 2016
B. Abbott; T. Adams; R. Bonnand; D. Buskulic; M. Ducrot; V. Germain; R. Gouaty; N. Letendre; F. Marion; A. Masserot; B. Mours; L. Rolland; D. Verkindt; M. Was; M. Yvert; G. Cagnoli; J. Degallaix; V. Dolique; R. Flaminio; M. Granata; D. Hofman; C. Michel; R. Pedurand; L. Pinard; B. Sassolas; N. Straniero; N. Arnaud; M. A. Bizouard; V. Brisson; J. Casanueva Diaz
The first observational run of the Advanced LIGO detectors, from September 12, 2015 to January 19, 2016, saw the first detections of gravitational waves from binary black hole mergers. In this paper we present full results from a search for binary black hole merger signals with total masses up to 100M⊙ and detailed implications from our observations of these systems. Our search, based on general-relativistic models of gravitational wave signals from binary black hole systems, unambiguously identified two signals, GW150914 and GW151226, with a significance of greater than 5σ over the observing period. It also identified a third possible signal, LVT151012, with substantially lower significance, which has a 87% probability of being of astrophysical origin. We provide detailed estimates of the parameters of the observed systems. Both GW150914 and GW151226 provide an unprecedented opportunity to study the two-body motion of a compact-object binary in the large velocity, highly nonlinear regime. We do not observe any deviations from general relativity, and place improved empirical bounds on several high-order post-Newtonian coefficients. From our observations we infer stellar-mass binary black hole merger rates lying in the range 9−240Gpc−3yr−1. These observations are beginning to inform astrophysical predictions of binary black hole formation rates, and indicate that future observing runs of the Advanced detector network will yield many more gravitational wave detections.
Physical Review Letters | 2016
B. Abbott; G. Cagnoli; J. Degallaix; V. Dolique; R. Flaminio; M. Granata; D. Hofman; C. Michel; R. Pedurand; L. Pinard; B. Sassolas; N. Straniero; T. Adams; R. Bonnand; D. Buskulic; M. Ducrot; V. Germain; R. Gouaty; N. Letendre; F. Marion; A. Masserot; B. Mours; L. Rolland; D. Verkindt; M. Was; M. Yvert; N. Arnaud; M. A. Bizouard; V. Brisson; J. Casanueva Diaz
On September 14, 2015, the Laser Interferometer Gravitational-Wave Observatory (LIGO) detected a gravitational-wave transient (GW150914); we characterize the properties of the source and its parameters. The data around the time of the event were analyzed coherently across the LIGO network using a suite of accurate waveform models that describe gravitational waves from a compact binary system in general relativity. GW150914 was produced by a nearly equal mass binary black hole of masses 36_{-4}^{+5}M_{⊙} and 29_{-4}^{+4}M_{⊙}; for each parameter we report the median value and the range of the 90% credible interval. The dimensionless spin magnitude of the more massive black hole is bound to be <0.7 (at 90% probability). The luminosity distance to the source is 410_{-180}^{+160} Mpc, corresponding to a redshift 0.09_{-0.04}^{+0.03} assuming standard cosmology. The source location is constrained to an annulus section of 610 deg^{2}, primarily in the southern hemisphere. The binary merges into a black hole of mass 62_{-4}^{+4}M_{⊙} and spin 0.67_{-0.07}^{+0.05}. This black hole is significantly more massive than any other inferred from electromagnetic observations in the stellar-mass regime.
Physical Review Letters | 2016
B. Abbott; G. Cagnoli; J. Degallaix; V. Dolique; R. Flaminio; M. Granata; D. Hofman; C. Michel; R. Pedurand; L. Pinard; B. Sassolas; N. Straniero; T. Adams; R. Bonnand; D. Buskulic; M. Ducrot; V. Germain; R. Gouaty; N. Letendre; F. Marion; A. Masserot; B. Mours; L. Rolland; D. Verkindt; M. Was; M. Yvert; N. Arnaud; M. A. Bizouard; V. Brisson; J. Casanueva Diaz
The LIGO detection of the gravitational wave transient GW150914, from the inspiral and merger of two black holes with masses
The Astrophysical Journal | 2016
B. Abbott; G. Cagnoli; J. Degallaix; V. Dolique; R. Flaminio; M. Granata; D. Hofman; C. Michel; R. Pedurand; L. Pinard; B. Sassolas; N. Straniero; T. Adams; R. Bonnand; D. Buskulic; M. Ducrot; V. Germain; R. Gouaty; N. Letendre; F. Marion; A. Masserot; B. Mours; L. Rolland; D. Verkindt; M. Was; M. Yvert; N. Arnaud; M. A. Bizouard; V. Brisson; J. Casanueva Diaz
\gtrsim 30\, \text{M}_\odot
Physical Review D | 2016
S. Adrián-Martínez; M. G. Aartsen; B. Abbott; T. Pradier; G. Cagnoli; J. Degallaix; V. Dolique; R. Flaminio; M. Granata; D. Hofman; C. Michel; R. Pedurand; L. Pinard; B. Sassolas; N. Straniero; J.-J. Aubert; V. Bertin; J. Brunner; J. Busto; J. Carr; H. Costantini; P. Coyle; D. Dornic; A. Mathieu; D. Turpin; C. Vallée; T. Adams; R. Bonnand; D. Buskulic; M. Ducrot
, suggests a population of binary black holes with relatively high mass. This observation implies that the stochastic gravitational-wave background from binary black holes, created from the incoherent superposition of all the merging binaries in the Universe, could be higher than previously expected. Using the properties of GW150914, we estimate the energy density of such a background from binary black holes. In the most sensitive part of the Advanced LIGO/Virgo band for stochastic backgrounds (near 25 Hz), we predict
Physical Review D | 2004
Maurice H. P. M. van Putten; Amir Levinson; Hyun Kyu Lee; T. Regimbau; Michele Punturo; G. M. Harry
\Omega_\text{GW}(f=25 Hz) = 1.1_{-0.9}^{+2.7} \times 10^{-9}
Astronomy and Astrophysics | 2001
T. Regimbau; J. A. de Freitas Pacheco
with 90\% confidence. This prediction is robustly demonstrated for a variety of formation scenarios with different parameters. The differences between models are small compared to the statistical uncertainty arising from the currently poorly constrained local coalescence rate. We conclude that this background is potentially measurable by the Advanced LIGO/Virgo detectors operating at their projected final sensitivity.
The Astrophysical Journal | 2011
X. J. Zhu; E. J. Howell; T. Regimbau; David Blair; Zong-Hong Zhu
A transient gravitational-wave signal, GW150914, was identified in the twin Advanced LIGO detectors on September 14, 2015 at 09:50:45 UTC. To assess the implications of this discovery, the detectors remained in operation with unchanged configurations over a period of 39 d around the time of the signal. At the detection statistic threshold corresponding to that observed for GW150914, our search of the 16 days of simultaneous two-detector observational data is estimated to have a false alarm rate (FAR) of < 4.9 × 10^(−6) yr^(−1), yielding a p-value for GW150914 of < 2 × 10^(−7). Parameter estimation followup on this trigger identifies its source as a binary black hole (BBH) merger with component masses (m_1, m_2) = (36^(+5)_(−4), 29^(+4)_(−4)) M_⊙ at redshift z = 0.09^(+0.03)_(−0.04) (median and 90\% credible range). Here we report on the constraints these observations place on the rate of BBH coalescences. Considering only GW150914, assuming that all BBHs in the Universe have the same masses and spins as this event, imposing a search FAR threshold of 1 per 100 years, and assuming that the BBH merger rate is constant in the comoving frame, we infer a 90% credible range of merger rates between 2--53 Gpc^(−3) yr^(−1) (comoving frame). Incorporating all search triggers that pass a much lower threshold while accounting for the uncertainty in the astrophysical origin of each trigger, we estimate a higher rate, ranging from 13--600 Gpc^(−3) yr^(−1) depending on assumptions about the BBH mass distribution. All together, our various rate estimates fall in the conservative range 2--600 Gpc^(−3) yr^(−1).
Astronomy and Astrophysics | 2006
T. Regimbau; J. A. de Freitas Pacheco
We present the high-energy-neutrino follow-up observations of the first gravitational wave transient GW150914 observed by the Advanced LIGO detectors on September 14, 2015. We search for coincident neutrino candidates within the data recorded by the IceCube and Antares neutrino detectors. A possible joint detection could be used in targeted electromagnetic follow-up observations, given the significantly better angular resolution of neutrino events compared to gravitational waves. We find no neutrino candidates in both temporal and spatial coincidence with the gravitational wave event. Within ±500 s of the gravitational wave event, the number of neutrino candidates detected by IceCube and Antares were three and zero, respectively. This is consistent with the expected atmospheric background, and none of the neutrino candidates were directionally coincident with GW150914. We use this nondetection to constrain neutrino emission from the gravitational-wave event.
Physical Review D | 2012
Chengjian Wu; V. Mandic; T. Regimbau
Gamma-ray bursts are believed to originate in core-collapse of massive stars. This produces an active nucleus containing a rapidly rotating Kerr black hole surrounded by a uniformly magnetized torus represented by two counter-oriented current rings. We quantify black hole spin-interactions with the torus and charged particles along open magnetic flux-tubes subtended by the event horizon. A major output of Egw=4e53 erg is radiated in gravitational waves of frequency fgw=500 Hz by a quadrupole mass-moment in the torus. Consistent with GRB-SNe, we find (i) Ts=90s (tens of s, Kouveliotou et al. 1993), (ii) aspherical SNe of kinetic energy Esn=2e51 erg (2e51 erg in SN1998bw, Hoeflich et al. 1999) and (iii) GRB-energies Egamma=2e50 erg (3e50erg in Frail et al. 2001). GRB-SNe occur perhaps about once a year within D=100Mpc. Correlating LIGO/Virgo detectors enables searches for nearby events and their spectral closure density 6e-9 around 250Hz in the stochastic background radiation in gravitational waves. At current sensitivity, LIGO-Hanford may place an upper bound around 150MSolar in GRB030329. Detection of Egw thus provides a method for identifying Kerr black holes by calorimetry.