J. K. Blackburn
California Institute of Technology
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Featured researches published by J. K. Blackburn.
Classical and Quantum Gravity | 2010
J. Abadie; R. Abbott; M. Abernathy; T. Accadia; F. Acernese; C. Adams; R. Adhikari; B. Allen; G. Allen; E. Amador Ceron; S. Anderson; Warren G. Anderson; F. Antonucci; S Aoudia; M. A. Arain; M. C. Araya; M. Aronsson; K G Arun; S. Aston; P. Astone; D. Atkinson; S. Babak; S. Ballmer; D. Barker; F. Barone; P. Barriga; L. Barsotti; M. Barsuglia; M. A. Barton; I. Bartos
We present an up-to-date, comprehensive summary of the rates for all types of compact binary coalescence sources detectable by the initial and advanced versions of the ground-based gravitational-wave detectors LIGO and Virgo. Astrophysical estimates for compact-binary coalescence rates depend on a number of assumptions and unknown model parameters and are still uncertain. The most confident among these estimates are the rate predictions for coalescing binary neutron stars which are based on extrapolations from observed binary pulsars in our galaxy. These yield a likely coalescence rate of 100 Myr−1 per Milky Way Equivalent Galaxy (MWEG), although the rate could plausibly range from 1 Myr−1 MWEG−1 to 1000 Myr−1 MWEG−1 (Kalogera et al 2004 Astrophys. J. 601 L179; Kalogera et al 2004 Astrophys. J. 614 L137 (erratum)). We convert coalescence rates into detection rates based on data from the LIGO S5 and Virgo VSR2 science runs and projected sensitivities for our advanced detectors. Using the detector sensitivities derived from these data, we find a likely detection rate of 0.02 per year for Initial LIGO–Virgo interferometers, with a plausible range between 2 × 10−4 and 0.2 per year. The likely binary neutron–star detection rate for the Advanced LIGO–Virgo network increases to 40 events per year, with a range between 0.4 and 400 per year.
The Astrophysical Journal | 2010
B. Abbott; R. Abbott; F. Acernese; R. Adhikari; P. Ajith; B. Allen; G. Allen; R. Amin; S. Anderson; W. G. Anderson; F. Antonucci; S. Aoudia; M. C. Araya; H. Armandula; P. Armor; K. G. Arun; Y. Aso; S. Aston; P. Astone; P. Aufmuth; C. Aulbert; S. Babak; P. Baker; G. Ballardin; S. Ballmer; C. Barker; D. Barker; F. Barone; B. Barr; P. Barriga
We present the results of a search for gravitational-wave bursts associated with 137 gamma-ray bursts (GRBs) that were detected by satellite-based gamma-ray experiments during the fifth LIGO science run and first Virgo science run. The data used in this analysis were collected from 2005 November 4 to 2007 October 1, and most of the GRB triggers were from the Swift satellite. The search uses a coherent network analysis method that takes into account the different locations and orientations of the interferometers at the three LIGO-Virgo sites. We find no evidence for gravitational-wave burst signals associated with this sample of GRBs. Using simulated short-duration (<1 s) waveforms, we set upper limits on the amplitude of gravitational waves associated with each GRB. We also place lower bounds on the distance to each GRB under the assumption of a fixed energy emission in gravitational waves, with typical limits of D ~ 15 Mpc (E_GW^iso / 0.01 M_o c^2)^1/2 for emission at frequencies around 150 Hz, where the LIGO-Virgo detector network has best sensitivity. We present astrophysical interpretations and implications of these results, and prospects for corresponding searches during future LIGO-Virgo runs.
The Astrophysical Journal | 2010
J. Abadie; B. Abbott; R. Abbott; M. Abernathy; C. Adams; R. Adhikari; P. Ajith; B. Allen; G. Allen; E. Amador Ceron; R. Amin; S. Anderson; W. G. Anderson; M. A. Arain; M. C. Araya; M. Aronsson; Y. Aso; S. Aston; D. Atkinson; P. Aufmuth; C. Aulbert; S. Babak; P. Baker; S. Ballmer; D. Barker; S. Barnum; B. Barr; P. Barriga; L. Barsotti; M. A. Barton
We present a search for periodic gravitational waves from the neutron star in the supernova remnant Cassiopeia A. The search coherently analyzes data in a 12 day interval taken from the fifth science run of the Laser Interferometer Gravitational-Wave Observatory. It searches gravitational-wave frequencies from 100 to 300 Hz and covers a wide range of first and second frequency derivatives appropriate for the age of the remnant and for different spin-down mechanisms. No gravitational-wave signal was detected. Within the range of search frequencies, we set 95% confidence upper limits of (0.7-1.2) × 10–24 on the intrinsic gravitational-wave strain, (0.4-4) × 10–4 on the equatorial ellipticity of the neutron star, and 0.005-0.14 on the amplitude of r-mode oscillations of the neutron star. These direct upper limits beat indirect limits derived from energy conservation and enter the range of theoretical predictions involving crystalline exotic matter or runaway r-modes. This paper is also the first gravitational-wave search to present upper limits on the r-mode amplitude.
Physical Review D | 2017
B. Abbott; R. Abbott; M. R. Abernathy; R. Adhikari; S. Anderson; K. Arai; M. C. Araya; J. C. Barayoga; B. Barish; B. K. Berger; G. Billingsley; J. K. Blackburn; R. Bork; A. F. Brooks; C. Cahillane; T. Callister; C. Cepeda; R. Chakraborty; T. Chalermsongsak; P. Couvares; D. C. Coyne; V. Dergachev; R. W. P. Drever; P. Ehrens; T. Etzel; S. E. Gossan; K. E. Gushwa; E. K. Gustafson; E. D. Hall; A. W. Heptonstall
In Advanced LIGO, detection and astrophysical source parameter estimation of the binary black hole merger GW150914 requires a calibrated estimate of the gravitational-wave strain sensed by the detectors. Producing an estimate from each detector’s differential arm length control loop readout signals requires applying time domain filters, which are designed from a frequency domain model of the detector’s gravitational-wave response. The gravitational-wave response model is determined by the detector’s opto-mechanical response and the properties of its feedback control system. The measurements used to validate the model and characterize its uncertainty are derived primarily from a dedicated photon radiation pressure actuator, with cross-checks provided by optical and radio frequency references. We describe how the gravitational-wave readout signal is calibrated into equivalent gravitational-wave-induced strain and how the statistical uncertainties and systematic errors are assessed. Detector data collected over 38 calendar days, from September 12 to October 20, 2015, contain the event GW150914 and approximately 16 days of coincident data used to estimate the event false alarm probability. The calibration uncertainty is less than 10% in magnitude and 10° in phase across the relevant frequency band, 20 Hz to 1 kHz.
Physical Review Letters | 1999
B. Allen; J. K. Blackburn; P. R. Brady; Jolien D. E. Creighton; T. D. Creighton; S. Droz; A. D. Gillespie; Scott A. Hughes; S. Kawamura; T. T. Lyons; J. E. Mason; B. J. Owen; F. J. Raab; M. W. Regehr; B. S. Sathyaprakash; R. L. Savage; S. E. Whitcomb; A. G. Wiseman
Using optimal matched filtering, we search 25 hours of data from the LIGO 40-m prototype laser interferometric gravitational-wave detector for gravitational-wave chirps emitted by coalescing binary systems within our Galaxy. This is the first test of this filtering technique on real interferometric data. An upper limit on the rate R of neutron star binary inspirals in our Galaxy is obtained: with 90% confidence, R<0.5h-1. Similar experiments with LIGO interferometers will provide constraints on the population of tight binary neutron star systems in the Universe.
Physical Review D | 2015
B. Abbott; R. Abbott; T. D. Abbott; M. Abernathy; F. Acernese; K. Ackley; C. Adams; T. Adams; P. Addesso; R. Adhikari; V. B. Adya; C. Affeldt; M. Agathos; K. Agatsuma; N. Aggarwal; O. D. Aguiar; A. Ain; P. Ajith; B. Allen; A. Allocca; D. Amariutei; S. Anderson; W. G. Anderson; Koji Arai; M. C. Araya; C. C. Arceneaux; J. S. Areeda; N. Arnaud; K. G. Arun; G. Ashton
We present the results of a search for long-duration gravitational wave transients in two sets of data collected by the LIGO Hanford and LIGO Livingston detectors between November 5, 2005 and September 30, 2007, and July 7, 2009 and October 20, 2010, with a total observational time of 283.0 days and 132.9 days, respectively. The search targets gravitational wave transients of duration 10 - 500 seconds in a frequency band of 40 - 1000 Hz, with minimal assumptions about the signal waveform, polarization, source direction, or time of occurrence. All candidate triggers were consistent with the expected background; as a result we set 90% confidence upper limits on the rate of long-duration gravitational wave transients for different types of gravitational wave signals. We also report upper limits on the source rate density per year per Mpc^3 for specific signal models. These are the first results from an all-sky search for unmodeled long-duration transient gravitational waves.
Classical and Quantum Gravity | 2002
P. Charlton; Stuart B. Anderson; J. K. Blackburn; J. A. Edlund; Fredrick A. Jenet; A. Lazzarini; Thomas A. Prince; Massimo Tinto; L. Wen
The fast chirp transform (FCT) provides a powerful formalism for the detection of signals with variable frequency, in much the same way that the Fourier transform provides a formalism for the detection of constant frequency signals. The FCT algorithm has significant applications in the detection of gravitational waves, particularly the gravitational wave signal produced by an inspiralling compact binary. We report on progress towards a parallelized search code to identify inspiral events in interferometer data and estimate the mass parameters.
Archive | 2012
J. Aasi; J. Abadie; B. Abbott; R. Abbott; T. D. Abbott; M. Abernathy; T. Accadia; F. Acernese; C. Adams; T. Adams; P. Addesso; R. Adhikari; C. Affeldt; M. Agathos; K. Agatsuma; P. Ajith; B. Allen; A. Allocca; E. Amador Ceron; D. Amariutei; S. Anderson; W. G. Anderson; Koji Arai; M. C. Araya; S. Ast; S. Aston; P. Astone; D. Atkinson; P. Aufmuth; C. Aulbert