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Dive into the research topics where E. K. Gustafson is active.

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Featured researches published by E. K. Gustafson.


Classical and Quantum Gravity | 2010

Effect of heat treatment on mechanical dissipation in Ta2O5 coatings

I. W. Martin; R. Bassiri; R. Nawrodt; Martin M. Fejer; A. M. Gretarsson; E. K. Gustafson; G. M. Harry; J. Hough; Ian MacLaren; S. Penn; S. Reid; R. Route; S. Rowan; C. Schwarz; P. Seidel; John Scott; Adam L. Woodcraft

Thermal noise arising from mechanical dissipation in dielectric reflective coatings is expected to critically limit the sensitivity of precision measurement systems such as high-resolution optical spectroscopy, optical frequency standards and future generations of interferometric gravitational wave detectors. We present measurements of the effect of post-deposition heat treatment on the temperature dependence of the mechanical dissipation in ion-beam sputtered tantalum pentoxide between 11 K and 300 K. We find that the temperature dependence of the dissipation is strongly dependent on the temperature at which the heat treatment was carried out, and we have identified three dissipation peaks occurring at different heat treatment temperatures. At temperatures below 200 K, the magnitude of the loss was found to increase with higher heat treatment temperatures, indicating that heat treatment is a significant factor in determining the level of coating thermal noise.


Physical Review D | 2002

Thermal noise in half-infinite mirrors with nonuniform loss: A slab of excess loss in a half-infinite mirror

Norio Nakagawa; A. M. Gretarsson; E. K. Gustafson; Martin M. Fejer

We calculate the thermal noise in half-infinite mirrors containing a layer of arbitrary thickness and depth made of excessively lossy material but with the same elastic material properties as the substrate. For the special case of a thin lossy layer on the surface of the mirror, the excess noise scales as the ratio of the coating loss to the substrate loss and as the ratio of the coating thickness to the laser beam spot size. Assuming a silica substrate with a loss function of 3x10-8 the coating loss must be less than 3x10-5 for a 6 cm spot size and a 7 micrometers thick coating to avoid increasing the spectral density of displacement noise by more than 10%. A similar number is obtained for sapphire test masses.


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 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 | 2014

Enhanced characteristics of fused silica fibers using laser polishing

A. Heptonstall; M. A. Barton; A. S. Bell; A Bohn; G. Cagnoli; A. Cumming; A. Grant; E. K. Gustafson; G. Hammond; J. Hough; R. Jones; R. Kumar; K Lee; I. W. Martin; N. A. Robertson; S. Rowan; K. A. Strain; K. V. Tokmakov

The search for gravitational wave signals from astrophysical sources has led to the current work to upgrade the two largest of the long-baseline laser interferometers, the LIGO detectors. The first fused silica mirror suspensions for the Advanced LIGO gravitational wave detectors have been installed at the LIGO Hanford and Livingston sites. These quadruple pendulums use synthetic fused silica fibers produced using a CO2 laser pulling machine to reduce thermal noise in the final suspension stage. The suspension thermal noise in Advanced LIGO is predicted to be limited by internal damping in the surface layer of the fibers, damping in the weld regions, and the strength of the fibers. We present here a new method for increasing the fracture strength of fused silica fibers by laser polishing of the stock material from which they are produced. We also show measurements of mechanical loss in laser polished fibers, showing a reduction of 30% in internal damping in the surface layer.


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.


Advanced Solid State Lasers (1999), paper MA4 | 2001

A 100 W edge-pumped Nd:YAG conduction-cooled slab laser

William M. Tulloch; Todd S. Rutherford; E. K. Gustafson; Robert L. Byer

We have demonstrated a 104 W multimode, laser-diode-pumped zig-zag slab laser based on conduction-cooling and a novel pumping geometry called edge-pumping. The advantages of the edge-pumped design include efficient pump absorption, conductive-cooling, power scalablity, and a simple opto-mechanical laser head design. The multimode laser operates at 104 W with 40% slope efficiency. TEM00 mode operation was demonstrated at 39.5 W for 250 W of pump power with a slope efficiency of 21%. Absorption loss due to the thermally populated lower laser level decreases the slope efficiency at high pump powers. This effect is included in laser oscillator performance models to accurately predict the operation of the oscillator.


Classical and Quantum Gravity | 2016

Passive, free-space heterodyne laser gyroscope

W. Z. Korth; A. Heptonstall; E. D. Hall; Koji Arai; E. K. Gustafson; R. Adhikari

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R. Adhikari

California Institute of Technology

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G. Billingsley

Massachusetts Institute of Technology

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A. Ananyeva

California Institute of Technology

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A. Heptonstall

California Institute of Technology

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B. Abbott

University of Oklahoma

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K. Arai

California Institute of Technology

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K. E. Gushwa

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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