Authors

Carl Blair, The University of Western Australia
Slawek Gras, Massachusetts Institute of Technology
Richard Abbott, California Institute of Technology
Stuart Aston, LIGO Livingston
Joseph Betzwieser, LIGO Livingston
David Blair, The University of Western Australia
Ryan Derosa, LIGO Livingston
Matthew Evans, Massachusetts Institute of Technology
Valera Frolov, LIGO Livingston
Peter Fritschel, Massachusetts Institute of Technology
Hartmut Grote, Max Planck Institute for Gravitational Physics (Albert Einstein Institute)
Terra Hardwick, Louisiana State University
Jian Liu, The University of Western Australia
Marc Lormand, LIGO Livingston
John Miller, Massachusetts Institute of Technology
Adam Mullavey, LIGO Livingston
Brian O'Reilly, LIGO Livingston
Chunnong Zhao, The University of Western Australia
B. P. Abbott, California Institute of TechnologyFollow
T. D. Abbott, Louisiana State UniversityFollow
C. Adams, American UniversityFollow
R. X. Adhikari, California Institute of TechnologyFollow
S. B. Anderson, California Institute of TechnologyFollow
A. Ananyeva, California Institute of TechnologyFollow
S. Appert, California Institute of Technology
K. Arai, California Institute of Technology
S. W. Ballmer, University of Florida
D. Barker, LIGO Livingston
B. Barr, Università degli Studi del Sannio
L. Barsotti, Max Planck Institute for Gravitational Physics (Albert Einstein Institute)
J. Bartlett, LIGO Livingston
I. Bartos, LIGO, Massachusetts Institute of Technology
J. C. Batch, LIGO Livingston

Document Type

Article

Publication Date

4-11-2017

Abstract

Interferometric gravitational wave detectors operate with high optical power in their arms in order to achieve high shot-noise limited strain sensitivity. A significant limitation to increasing the optical power is the phenomenon of three-mode parametric instabilities, in which the laser field in the arm cavities is scattered into higher-order optical modes by acoustic modes of the cavity mirrors. The optical modes can further drive the acoustic modes via radiation pressure, potentially producing an exponential buildup. One proposed technique to stabilize parametric instability is active damping of acoustic modes. We report here the first demonstration of damping a parametrically unstable mode using active feedback forces on the cavity mirror. A 15 538 Hz mode that grew exponentially with a time constant of 182 sec was damped using electrostatic actuation, with a resulting decay time constant of 23 sec. An average control force of 0.03 nN was required to maintain the acoustic mode at its minimum amplitude.

Publication Source (Journal or Book title)

Physical Review Letters

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