A. Effler
California Institute of Technology
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Featured researches published by A. Effler.
Physical Review Letters | 2015
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.
Review of Scientific Instruments | 2016
C. L. Mueller; M. A. Arain; G. Ciani; R. T. Derosa; A. Effler; D. Feldbaum; V. V. Frolov; P. Fulda; J. Gleason; M. C. Heintze; Keita Kawabe; E. J. King; K. Kokeyama; W. Z. Korth; R. M. Martin; A. Mullavey; Jan Peold; V. Quetschke; D. H. Reitze; D. B. Tanner; C. Vorvick; L. Williams; G. Mueller
The advanced LIGO gravitational wave detectors are nearing their design sensitivity and should begin taking meaningful astrophysical data in the fall of 2015. These resonant optical interferometers will have unprecedented sensitivity to the strains caused by passing gravitational waves. The input optics play a significant part in allowing these devices to reach such sensitivities. Residing between the pre-stabilized laser and the main interferometer, the input optics subsystem is tasked with preparing the laser beam for interferometry at the sub-attometer level while operating at continuous wave input power levels ranging from 100 mW to 150 W. These extreme operating conditions required every major component to be custom designed. These designs draw heavily on the experience and understanding gained during the operation of Initial LIGO and Enhanced LIGO. In this article, we report on how the components of the input optics were designed to meet their stringent requirements and present measurements showing how well they have lived up to their design.
Classical and Quantum Gravity | 2014
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.
Classical and Quantum Gravity | 2015
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 | 2014
E. Thrane; N. Christensen; Robert M. S. Schofield; A. Effler
One of the key science goals of advanced gravitational-wave detectors is to observe a stochastic gravitational-wave background. However, recent work demonstrates that correlated magnetic fields from Schumann resonances can produce correlated strain noise over global distances, potentially limiting the sensitivity of stochastic background searches with advanced detectors. In this paper, we estimate the correlated noise budget for the worldwide advanced detector network and conclude that correlated noise may affect upcoming measurements. We investigate the possibility of a Wiener filtering scheme to subtract correlated noise from Advanced LIGO searches, and estimate the required specifications. We also consider the possibility that residual correlated noise remains following subtraction, and we devise an optimal strategy for measuring astronomical parameters in the presence of correlated noise. Using this new formalism, we estimate the loss of sensitivity for a broadband, isotropic stochastic background search using 1 yr of LIGO data at design sensitivity. Given our current noise budget, the uncertainty with which LIGO can estimate energy density will likely increase by a factor of ≈12 —if it is impossible to achieve significant subtraction. Additionally, narrow band cross-correlation searches may be severely affected at low frequencies f≲70 Hz without effective subtraction.
Physical Review D | 2018
M. W. Coughlin; Melissa A. Guidry; Andrzej Kulak; I. Fiori; F. Paoletti; Jacobo Salvador; E. Thrane; Mark Golkowski; Yuu Kataoka; N. Christensen; J. Harms; Tsutomu Ogawa; K. Hayama; V. Boschi; A. Chincarini; Sho Atsuta; Robert M. S. Schofield; Michael Laxen; Janusz Mlynarczyk; Kentaro Somiya; Alessio Cirone; P. M. Meyers; A. Effler; Jerzy Kubisz; Andrew Matas; Rosario De Rosa
Correlated magnetic noise from Schumann resonances threatens to contaminate the observation of a stochastic gravitational-wave background in interferometric detectors. In previous work, we reported on the first effort to eliminate global correlated noise from the Schumann resonances using Wiener filtering, demonstrating as much as a factor of two reduction in the coherence between magnetometers on different continents. In this work, we present results from dedicated magnetometer measurements at the Virgo and KAGRA sites, which are the first results for subtraction using data from gravitational-wave detector sites. We compare these measurements to a growing network of permanent magnetometer stations, including at the LIGO sites. We show the effect of mutual magnetometer attraction, arguing that magnetometers should be placed at least one meter from one another. In addition, for the first time, we show how dedicated measurements by magnetometers near to the interferometers can reduce coherence to a level consistent with uncorrelated noise, making a potential detection of a stochastic gravitational-wave background possible.
Optics Express | 2015
A. Staley; D. Hoak; A. Effler; K. Izumi; S. Dwyer; K. Kawabe; E. J. King; M. Rakhmanov; R. L. Savage; D. Sigg
We use doubly phase modulated light to measure both the length and the linewidth of an optical resonator with high precision. The first modulation is at RF frequencies and is set near a multiple of the free spectral range, whereas the second modulation is at audio frequencies to eliminate offset errors at DC. The light in transmission or in reflection of the optical resonator is demodulated while sweeping the RF frequency over the optical resonance. We derive expressions for the demodulated power in transmission, and show that the zero crossings of the demodulated signal in transmission serve as a precise measure of the cavity linewidth at half maximum intensity. We demonstrate the technique on two resonant cavities, with lengths 16 m and a 4 km, and achieve an absolute length accuracy as low as 70 ppb. The cavity width for the 16 m cavity was determined with an accuracy of approximately 6000 ppm. Through an analysis of the systematic errors we show that this result could be substantially improved with the reduction of technical sources of uncertainty.
Classical and Quantum Gravity | 2015
A. Effler; R. Schofield; V. V. Frolov; G. González; K. Kawabe; J. R. Smith; J. Birch; R. McCarthy
Bulletin of the American Physical Society | 2016
D. B. Tanner; Arain; G. Ciani; D. Feldbaum; P. Fulda; J. Gleason; R. Goetz; M. C. Heintze; R. M. Martin; C. L. Mueller; L. Williams; G. Mueller; V. Quetschke; W. Z. Korth; D. H. Reitze; R. T. Derosa; A. Effler; K. Kokeyama; V. V. Frolov; A. Mullavey; J. Poeld