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Phys. Rev. D 78, 122002 (2008) [35 pages]

Atomic gravitational wave interferometric sensor

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Savas Dimopoulos1,*, Peter W. Graham2,†, Jason M. Hogan1,‡, Mark A. Kasevich1,§, and Surjeet Rajendran1,2,**
1Department of Physics, Stanford University, Stanford, California 94305, USA
2SLAC, Stanford University, Menlo Park, California 94025, USA

Received 28 August 2008; published 19 December 2008

We propose two distinct atom interferometer gravitational wave detectors, one terrestrial and another satellite based, utilizing the core technology of the Stanford 10 m atom interferometer presently under construction. Each configuration compares two widely separated atom interferometers run using common lasers. The signal scales with the distance between the interferometers, which can be large since only the light travels over this distance, not the atoms. The terrestrial experiment with two ∼10  m atom interferometers separated by a ∼1  km baseline can operate with strain sensitivity ∼10-19/√Hz in the 1 Hz–10 Hz band, inaccessible to LIGO, and can detect gravitational waves from solar mass binaries out to megaparsec distances. The satellite experiment with two atom interferometers separated by a ∼1000  km baseline can probe the same frequency spectrum as LISA with comparable strain sensitivity ∼10-20/√Hz. The use of ballistic atoms (instead of mirrors) as inertial test masses improves systematics coming from vibrations and acceleration noise, and significantly reduces spacecraft control requirements. We analyze the backgrounds in this configuration and discuss methods for controlling them to the required levels.

© 2008 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevD.78.122002
DOI:
10.1103/PhysRevD.78.122002
PACS:
04.80.−y, 03.75.Dg, 04.80.Nn, 95.55.Ym

*savas@stanford.edu

pwgraham@stanford.edu

hogan@stanford.edu

§kasevich@stanford.edu

**surjeet@stanford.edu

See Also

Comment: Peter L. Bender, Comment on “Atomic gravitational wave interferometric sensor”, Phys. Rev. D 84, 028101 (2011).