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Dive into the research topics where K. Arai is active.

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Featured researches published by K. Arai.


Astronomy and Astrophysics | 2012

Implementation and testing of the first prompt search for gravitational wave transients with electromagnetic counterparts

J. Abadie; B. Abbott; R. Abbott; T. D. Abbott; M. Abernathy; T. Accadia; F. Acernese; C. Adams; R. Adhikari; C. Affeldt; M. Agathos; P. Ajith; B. Allen; G. Allen; E. Amador Ceron; D. Amariutei; R. Amin; S. Anderson; W. G. Anderson; K. Arai; M. A. Arain; M. C. Araya; S. Aston; P. Astone; D. Atkinson; P. Aufmuth; C. Aulbert; B. E. Aylott; S. Babak; P. Baker

Aims. A transient astrophysical event observed in both gravitational wave (GW) and electromagnetic (EM) channels would yield rich scientific rewards. A first program initiating EM follow-ups to possible transient GW events has been developed and exercised by the LIGO and Virgo community in association with several partners. In this paper, we describe and evaluate the methods used to promptly identify and localize GW event candidates and to request images of targeted sky locations. Methods. During two observing periods (Dec. 17, 2009 to Jan. 8, 2010 and Sep. 2 to Oct. 20, 2010), a low-latency analysis pipeline was used to identify GW event candidates and to reconstruct maps of possible sky locations. A catalog of nearby galaxies and Milky Way globular clusters was used to select the most promising sky positions to be imaged, and this directional information was delivered to EM observatories with time lags of about thirty minutes. A Monte Carlo simulation has been used to evaluate the low-latency GW pipelines ability to reconstruct source positions correctly. Results. For signals near the detection threshold, our low-latency algorithms often localized simulated GW burst signals to tens of square degrees, while neutron star/neutron star inspirals and neutron star/black hole inspirals were localized to a few hundred square degrees. Localization precision improves for moderately stronger signals. The correct sky location of signals well above threshold and originating from nearby galaxies may be observed with similar to 50% or better probability with a few pointings of wide-field telescopes.Aims. A transient astrophysical event observed in both gravitational wave (GW) and electromagnetic (EM) channels would yield rich scientific rewards. A first program initiating EM follow-ups to possible transient GW events has been developed and exercised by the LIGO and Virgo community in association with several partners. In this paper, we describe and evaluate the methods used to promptly identify and localize GW event candidates and to request images of targeted sky locations. Methods. During two observing periods (Dec 17 2009 to Jan 8 2010 and Sep 2 to Oct 20 2010), a low-latency analysis pipeline was used to identify GW event candidates and to reconstruct maps of possible sky locations. A catalog of nearby galaxies and Milky Way globular clusters was used to select the most promising sky positions to be imaged, and this directional information was delivered to EM observatories with time lags of about thirty minutes. A Monte Carlo simulation has been used to evaluate the low-latency GW pipelines ability to reconstruct source positions correctly. Results. For signals near the detection threshold, our low-latency algorithms often localized simulated GW burst signals to tens of square degrees, while neutron star/neutron star inspirals and neutron star/black hole inspirals were localized to a few hundred square degrees. Localization precision improves for moderately stronger signals. The correct sky location of signals well above threshold and originating from nearby galaxies may be observed with ~50% or better probability with a few pointings of wide-field telescopes.


Physical Review D | 2017

Calibration of the Advanced LIGO detectors for the discovery of the binary black-hole merger GW150914

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.


Classical and Quantum Gravity | 2014

Achieving resonance in the Advanced LIGO gravitational-wave interferometer

A. Staley; D. V. Martynov; R. Abbott; R. Adhikari; K. Arai; S. Ballmer; L. Barsotti; A. F. Brooks; R. T. Derosa; S. Dwyer; A. Effler; M. Evans; P. Fritschel; V. V. Frolov; C. Gray; C. Guido; R. Gustafson; M. C. Heintze; D. Hoak; K. Izumi; K. Kawabe; E. J. King; J. S. Kissel; K. Kokeyama; M. Landry; D. E. McClelland; J. Miller; A. Mullavey; B OʼReilly; J. G. Rollins

Interferometric gravitational-wave detectors are complex instruments comprised of a Michelson interferometer enhanced by multiple coupled cavities. Active feedback control is required to operate these instruments and keep the cavities locked on resonance. The optical response is highly nonlinear until a good operating point is reached. The linear operating range is between 0.01% and 1% of a fringe for each degree of freedom. The resonance lock has to be achieved in all five degrees of freedom simultaneously, making the acquisition difficult. Furthermore, the cavity linewidth seen by the laser is only _(~1) Hz, which is four orders of magnitude smaller than the linewidth of the free running laser. The arm length stabilization system is a new technique used for arm cavity locking in Advanced LIGO. Together with a modulation technique utilizing third harmonics to lock the central Michelson interferometer, the Advanced LIGO detector has been successfully locked and brought to an operating point where detecting gravitational-waves becomes feasible.


Physical Review D | 2017

All-sky search for periodic gravitational waves in the O1 LIGO data

B. Abbott; R. Abbott; R. Adhikari; A. Ananyeva; S. Anderson; S. Appert; K. Arai; M. C. Araya; J. C. Barayoga; B. C. Barish; B. K. Berger; G. Billingsley; J. K. Blackburn; R. Bork; A. F. Brooks; S. Brunett; C. Cahillane; T. A. Callister; C. B. Cepeda; P. Couvares; D. C. Coyne; R. W. P. Drever; P. Ehrens; J. Eichholz; T. Etzel; J. Feicht; E. M. Fries; S. E. Gossan; K. E. Gushwa; E. K. Gustafson

We report on an all-sky search for periodic gravitational waves in the frequency band 20–475 Hz and with a frequency time derivative in the range of [−1.0,+0.1]×10−8u2009u2009Hz/s. Such a signal could be produced by a nearby spinning and slightly nonaxisymmetric isolated neutron star in our galaxy. This search uses the data from Advanced LIGO’s first observational run, O1. No periodic gravitational wave signals were observed, and upper limits were placed on their strengths. The lowest upper limits on worst-case (linearly polarized) strain amplitude h0 are ∼4×10−25 near 170 Hz. For a circularly polarized source (most favorable orientation), the smallest upper limits obtained are ∼1.5×10−25. These upper limits refer to all sky locations and the entire range of frequency derivative values. For a population-averaged ensemble of sky locations and stellar orientations, the lowest upper limits obtained for the strain amplitude are ∼2.5×10−25.


Physical Review D | 2017

Search for intermediate mass black hole binaries in the first observing run of Advanced LIGO

B. Abbott; R. Abbott; R. Adhikari; A. Ananyeva; S. Anderson; S. Appert; K. Arai; M. C. Araya; J. C. Barayoga; B. C. Barish; B. K. Berger; G. Billingsley; J. K. Blackburn; R. Bork; A. F. Brooks; S. Brunett; C. Cahillane; T. A. Callister; C. B. Cepeda; P. Couvares; D. C. Coyne; Ronald W. P. Drever; P. Ehrens; J. Eichholz; T. Etzel; J. Feicht; E. M. Fries; S. E. Gossan; K. E. Gushwa; E. K. Gustafson

During their first observational run, the two Advanced LIGO detectors attained an unprecedented sensitivity, resulting in the first direct detections of gravitational-wave signals produced by stellar-mass binary black hole systems. This paper reports on an all-sky search for gravitational waves (GWs) from merging intermediate mass black hole binaries (IMBHBs). The combined results from two independent search techniques were used in this study: the first employs a matched-filter algorithm that uses a bank of filters covering the GW signal parameter space, while the second is a generic search for GW transients (bursts). No GWs from IMBHBs were detected; therefore, we constrain the rate of several classes of IMBHB mergers. The most stringent limit is obtained for black holes of individual mass 100u2009u2009M⊙, with spins aligned with the binary orbital angular momentum. For such systems, the merger rate is constrained to be less than 0.93u2009u2009Gpc^(−3)u2009yr^(−1) in comoving units at the 90% confidence level, an improvement of nearly 2 orders of magnitude over previous upper limits.


Review of Scientific Instruments | 2016

An instrument to measure mechanical up-conversion phenomena in metals in the elastic regime

G. Vajente; E. A. Quintero; Xiaoyue Ni; K. Arai; E. K. Gustafson; N. A. Robertson; E. Sanchez; Julia R. Greer; R. Adhikari

Crystalline materials, such as metals, are known to exhibit deviation from a simple linear relation between strain and stress when the latter exceeds the yield stress. In addition, it has been shown that metals respond to varying external stress in a discontinuous way in this regime, exhibiting discrete releases of energy. This crackling noise has been extensively studied both experimentally and theoretically when the metals are operating in the plastic regime. In our study, we focus on the behavior of metals in the elastic regime, where the stresses are well below the yield stress. We describe an instrument that aims to characterize non-linear mechanical noise in metals when stressed in the elastic regime. In macroscopic systems, this phenomenon is expected to manifest as a non-stationary noise modulated by external disturbances applied to the material, a form of mechanical up-conversion of noise. The main motivation for this work is for the case of maraging steel components (cantilevers and wires) in the suspension systems of terrestrial gravitational wave detectors. Such instruments are planned to reach very ambitious displacement sensitivities, and therefore mechanical noise in the cantilevers could prove to be a limiting factor for the detectors final sensitivities, mainly due to non-linear up-conversion of low frequency residual seismic motion to the frequencies of interest for the gravitational wave observations. We describe here the experimental setup, with a target sensitivity of 10(-15) m/Hz in the frequency range of 10-1000 Hz, a simple phenomenological model of the non-linear mechanical noise, and the analysis method that is inspired by this model.

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R. Adhikari

California Institute of Technology

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R. Abbott

California Institute of Technology

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B. Abbott

University of Oklahoma

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E. K. Gustafson

California Institute of Technology

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M. C. Araya

California Institute of Technology

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S. Anderson

California Institute of Technology

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A. F. Brooks

Tata Institute of Fundamental Research

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C. Cahillane

University of Wisconsin–Milwaukee

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G. Billingsley

Massachusetts Institute of Technology

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J. C. Barayoga

California Institute of Technology

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