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Featured researches published by G. Vajente.


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.


Physical Review Letters | 2015

Observation of Parametric Instability in Advanced LIGO

M. Evans; Slawek Gras; P. Fritschel; John B. Miller; L. Barsotti; D. V. Martynov; A. F. Brooks; D. C. Coyne; R. Abbott; R. Adhikari; Koji Arai; Rolf Bork; Bill Kells; J. G. Rollins; N. D. Smith-Lefebvre; G. Vajente; Hiroaki Yamamoto; C. Adams; S. M. Aston; Joseph Betzweiser; V. V. Frolov; Adam Mullavey; A. Pele; J. H. Romie; M. Thomas; Keith Thorne; S. Dwyer; K. Izumi; Keita Kawabe; D. Sigg

Parametric instabilities have long been studied as a potentially limiting effect in high-power interferometric gravitational wave detectors. Until now, however, these instabilities have never been observed in a kilometer-scale interferometer. In this Letter, we describe the first observation of parametric instability in a gravitational wave detector, and the means by which it has been removed as a barrier to progress.


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]×10−8  Hz/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 100  M⊙, with spins aligned with the binary orbital angular momentum. For such systems, the merger rate is constrained to be less than 0.93  Gpc^(−3) yr^(−1) in comoving units at the 90% confidence level, an improvement of nearly 2 orders of magnitude over previous upper limits.


Classical and Quantum Gravity | 2015

Improving the data quality of Advanced LIGO based on early engineering run results

L. K. Nuttall; T. J. Massinger; J. S. Areeda; J. Betzwieser; S. Dwyer; A. Effler; Rebecca Fisher; P. Fritschel; J. S. Kissel; A. P. Lundgren; D. M. Macleod; D. V. Martynov; J. McIver; A. Mullavey; D. Sigg; J. R. Smith; G. Vajente; A. R. Williamson; C. C. Wipf

The Advanced Laser Interferometer Gravitational-wave Observatory (LIGO) detectors have completed their initial upgrade phase and will enter the first observing run in late 2015, with detector sensitivity expected to improve in future runs. Through the combined efforts of on-site commissioners and the Detector Characterization group of the LIGO Scientific Collaboration, interferometer performance, in terms of data quality, at both LIGO observatories has vastly improved from the start of commissioning efforts to present. Advanced LIGO has already surpassed Enhanced LIGO in sensitivity, and the rate of noise transients, which would negatively impact astrophysical searches, has improved. Here we give details of some of the work which has taken place to better the quality of the LIGO data ahead of the first observing run.


Physical Review D | 2018

Identification and mitigation of narrow spectral artifacts that degrade searches for persistent gravitational waves in the first two observing runs of Advanced LIGO

P. B. Covas; T. Callister; M. W. Coughlin; J. McIver; B. Abbott; R. Abbott; R. Adhikari; A. Ananyeva; S. Appert; K. Arai; G. Billingsley; R. Bork; A. F. Brooks; D. C. Coyne; T. Etzel; K. E. Gushwa; E. K. Gustafson; A. Heptonstall; W. Z. Korth; E. Maros; T. J. Massinger; F. Matichard; G. McIntyre; E. A. Quintero; D. H. Reitze; N. A. Robertson; J. G. Rollins; E. Sanchez; L. E. Sanchez; Robert W. Taylor

Searches are under way in Advanced LIGO and Virgo data for persistent gravitational waves from continuous sources, e.g. rapidly rotating galactic neutron stars, and stochastic sources, e.g. relic gravitational waves from the Big Bang or superposition of distant astrophysical events such as mergers of black holes or neutron stars. These searches can be degraded by the presence of narrow spectral artifacts (lines) due to instrumental or environmental disturbances. We describe a variety of methods used for finding, identifying and mitigating these artifacts, illustrated with particular examples. Results are provided in the form of lists of line artifacts that can safely be treated as non-astrophysical. Such lists are used to improve the efficiencies and sensitivities of continuous and stochastic gravitational wave searches by allowing vetoes of false outliers and permitting data cleaning.


Review of Scientific Instruments | 2017

A high throughput instrument to measure mechanical losses in thin film coatings

G. Vajente; A. Ananyeva; G. Billingsley; E. K. Gustafson; A. Heptonstall; E. Sanchez; C. I. Torrie

Brownian thermal noise generated by mechanical losses in thin film coatings limits the sensitivity of gravitational wave detectors, as well as several high precision metrology experiments. Improving the sensitivity of the next generation of gravitational wave detectors will require optical coatings with significantly reduced mechanical losses. In this paper, we describe a system that we developed to measure the mechanical loss angle of thin film coatings deposited on fused silica substrates. The novelty of this system resides in the capability of parallel measurement of up to four samples and the ability to simultaneously probe all the resonant modes of each sample. This high throughput measurement system allows the exploration of a large number of deposition and material parameters, which can be tuned to achieve low loss coatings.


Archive | 2014

Readout, Sensing, and Control

G. Vajente

Suspending the mirrors is one of the most crucial tasks in gravitational wave interferometer technology. The performance of the suspensions must provide the required attenuation of seismic noise and reduction of thermal noise, two fundamental limits to the sensitivity of any gravitational wave detector. Moreover, the suspension system must be equipped with sensors and actuators which are used to actively control some relevant degrees of freedom, so to be able to keep the interferometer at its working point (i.e., “locked”). In the first part of this chapter we deal with the basic principles behind the super attenuator chains developed in Virgo to reduce the seismic noise. In the second part, we illustrate the techniques to suspend the mirror reducing the thermal noise in the detection bandwidth, according to the theory illustrated in Chap. 8.


Classical and Quantum Gravity | 2014

Full modal simulation of opto-mechanical effects in optical systems

G. Vajente

The interaction of light with optical elements via radiation pressure plays a predominant role in determining the dynamics of many optical configurations, in particular when the mirrors composing the system have small masses or the light power is large. Gravitational wave interferometric detectors fall in the second category: opto-mechanical effects have been measured in first generation instruments and will be very relevant in second and third generations. So far, radiation pressure effects were studied using analytical models or simulation tools which were limited to specific optical systems or low order Hermite–Gauss modes. In this paper we present the first tool, to our knowledge, capable of a complete Hermite–Gauss modal simulation of radiation pressure induced effects, based on the modal interferometer simulation toolbox (MIST), described in details in a previous paper. This tool opens the possibility of the simulation of radiation pressure effects in realistic interferometric systems that include beam and optical element aberrations. The application of this tool to gravitational wave detectors will allow to better understand the incidence of realistic optical defects on the instrument operation and sensitivity. We also expect that this tool will be useful outside the gravitational wave community, for application on interferometric systems where radiation pressure dynamics is dominant, such as opto-mechanically-induced transparency, light mirror cavities and membrane-in-a-cavity systems. In this paper we describe the formalism used to implement radiation pressure in the MIST simulation tool and we give some example applications, including the first results on parametric instabilities in Fabry–Perot cavities based on a complete modal optical simulation.

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R. Adhikari

California Institute of Technology

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A. Ananyeva

California Institute of Technology

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E. K. Gustafson

California Institute of Technology

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G. Billingsley

California Institute of Technology

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R. Abbott

California Institute of Technology

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A. F. Brooks

Tata Institute of Fundamental Research

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K. Arai

California Institute of Technology

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B. Abbott

University of Oklahoma

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K. E. Gushwa

California Institute of Technology

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