J. Gleason
University of Florida
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Featured researches published by J. Gleason.
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.
Physical Review Letters | 2018
N. Du; N. Force; R. Khatiwada; E. Lentz; R. S. Ottens; L.J. Rosenberg; G. Rybka; G. Carosi; N. Woollett; D. Bowring; A. S. Chou; A. Sonnenschein; W. Wester; C. Boutan; N. S. Oblath; Richard Bradley; E. J. Daw; A. V. Dixit; John Clarke; S. O’Kelley; N. Crisosto; J. Gleason; S. Jois; P. Sikivie; I. Stern; N. S. Sullivan; D. B. Tanner; G. C. Hilton
This Letter reports the results from a haloscope search for dark matter axions with masses between 2.66 and 2.81 μeV. The search excludes the range of axion-photon couplings predicted by plausible models of the invisible axion. This unprecedented sensitivity is achieved by operating a large-volume haloscope at subkelvin temperatures, thereby reducing thermal noise as well as the excess noise from the ultralow-noise superconducting quantum interference device amplifier used for the signal power readout. Ongoing searches will provide nearly definitive tests of the invisible axion model over a wide range of axion masses.
Applied Optics | 2007
M. A. Arain; V. Quetschke; J. Gleason; L. Williams; M. Rakhmanov; Jinho Lee; Rachel J. Cruz; G. Mueller; D. B. Tanner; D. H. Reitze
We describe an adaptive optical system for use as a tunable focusing element. The system provides adaptive beam shaping via controlled thermal lensing in the optical elements. The system is agile, remotely controllable, touch free, and vacuum compatible; it offers a wide dynamic range, aberration-free focal length tuning, and can provide both positive and negative lensing effects. Focusing is obtained through dynamic heating of an optical element by an external pump beam. The system is especially suitable for use in interferometric gravitational wave interferometers employing high laser power, allowing for in situ control of the laser modal properties and compensation for thermal lensing of the primary laser. Using CO(2) laser heating of fused-silica substrates, we demonstrate a focal length variable from infinity to 4.0 m, with a slope of 0.082 diopter/W of absorbed heat. For on-axis operation, no higher-order modes are introduced by the adaptive optical element. Theoretical modeling of the induced optical path change and predicted thermal lens agrees well with measurement.
Optics Letters | 2006
V. Quetschke; J. Gleason; M. Rakhmanov; Jennifer A. Lee; L. Zhang; K. Yoshiki Franzen; C. Leidel; G. Mueller; R. Amin; D. B. Tanner; D. H. Reitze
An adaptive optical system for precise control of a laser beams mode structure has been developed. The system uses a dynamic lens based on controlled optical path deformation in a dichroic optical element that is heated with an auxiliary laser. Our method is essentially aberration free, has high dynamic range, and can be implemented with high average power laser beams where other adaptive optics methods fail. A quantitative model agrees well with our experimental data and demonstrates the potential of our method as a mode-matching and beam-shaping element for future large-scale gravitational wave detectors.
Review of Scientific Instruments | 2016
S. Karki; D. Tuyenbayev; S. Kandhasamy; B. Abbott; T. D. Abbott; E. H. Anders; J. M. Berliner; J. Betzwieser; C. Cahillane; L. Canete; C. Conley; H. P. Daveloza; N. De Lillo; J. Gleason; E. Goetz; K. Izumi; J. S. Kissel; G. Mendell; V. Quetschke; M. Rodruck; S. Sachdev; T. Sadecki; P. Schwinberg; A. Sottile; M. Wade; A. J. Weinstein; M. West; R. Savage
The two interferometers of the Laser Interferometry Gravitational-wave Observatory (LIGO) recently detected gravitational waves from the mergers of binary black hole systems. Accurate calibration of the output of these detectors was crucial for the observation of these events and the extraction of parameters of the sources. The principal tools used to calibrate the responses of the second-generation (Advanced) LIGO detectors to gravitational waves are systems based on radiation pressure and referred to as photon calibrators. These systems, which were completely redesigned for Advanced LIGO, include several significant upgrades that enable them to meet the calibration requirements of second-generation gravitational wave detectors in the new era of gravitational-wave astronomy. We report on the design, implementation, and operation of these Advanced LIGO photon calibrators that are currently providing fiducial displacements on the order of 10-18m/Hz with accuracy and precision of better than 1%.
Physical Review D | 2016
J. Hoskins; N. Crisosto; J. Gleason; P. Sikivie; I. Stern; N. S. Sullivan; D. B. Tanner; C. Boutan; M. Hotz; R. Khatiwada; D. Lyapustin; A. Malagon; R. S. Ottens; L.J. Rosenberg; G. Rybka; J.V. Sloan; A. Wagner; D. Will; G. Carosi; D. Carter; Leanne D. Duffy; Richard Bradley; John Clarke; S. O’Kelley; K. van Bibber; E. J. Daw
Non-virialized dark-matter axions may be present in the Milky Way halo in the form of low-velocity-dispersion flows. The Axion Dark Matter eXperiment performed a search for the conversion of these axions into microwave photons using a resonant cavity immersed in a strong, static magnetic field. The spread of photon energy in these measurements was measured at spectral resolutions of the order of 1 Hz and below. If the energy variation were this small, the frequency modulation of any real axion signal due to the orbital and rotational motion of the Earth would become non-negligible. Conservative estimates of the expected signal modulation were made and used as a guide for the search procedure. The photon frequencies covered by this search are 812
Review of Scientific Instruments | 2016
G. Ciani; M. A. Arain; S. Aston; D. Feldbaum; P. Fulda; J. Gleason; M. C. Heintze; R. M. Martin; C. L. Mueller; D. Nanda Kumar; A. Pele; D. H. Reitze; P. Sainathan; D. B. Tanner; L. Williams; G. Mueller
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Proceedings of SPIE | 2005
V. Quetschke; J. Gleason; Christina Leidel; Michelle Snider; Jinho Lee; M. Rakhmanov; Liang Zhang; G. Mueller; D. H. Reitze; D. B. Tanner
852 and 858
Physics of the Dark Universe | 2016
J.V. Sloan; M. Hotz; C. Boutan; Richard Bradley; G. Carosi; D. Carter; John Clarke; N. Crisosto; E. J. Daw; J. Gleason; J. Hoskins; R. Khatiwada; D. Lyapustin; A. Malagon; S. O’Kelley; R.S. Ottens; L.J. Rosenberg; G. Rybka; I. Stern; N. S. Sullivan; D. B. Tanner; K. van Bibber; A. Wagner; D. Will
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Bulletin of the American Physical Society | 2018
Ayman Hallal; Giuseppe Messineo; J. Gleason; D. B. Tanner; G. Mueller
892 MHz, which correspond to an axion mass of 3.36