Authors

B. Abbott, California Institute of Technology
R. Abbott, LIGO Livingston
R. Adhikari, Massachusetts Institute of Technology
A. Ageev, Lomonosov Moscow State University
B. Allen, University of Wisconsin-Milwaukee
R. Amin, University of Florida
S. B. Anderson, California Institute of Technology
W. G. Anderson, University of Texas at Brownsville and Texas Southmost College
M. Araya, California Institute of Technology
H. Armandula, California Institute of Technology
M. Ashley, Pennsylvania State University
F. Asiri, California Institute of Technology
P. Aufmuth, Gottfried Wilhelm Leibniz Universität Hannover
C. Aulbert, Max Planck Institute for Gravitational Physics (Albert Einstein Institute)
S. Babak, Cardiff University
R. Balasubramanian, Cardiff University
S. Ballmer, Massachusetts Institute of Technology
B. C. Barish, California Institute of Technology
C. Barker, LIGO Hanford
D. Barker, LIGO Hanford
M. Barnes, California Institute of Technology
B. Barr, University of Glasgow
M. A. Barton, California Institute of Technology
K. Bayer, Massachusetts Institute of Technology
R. Beausoleil, Stanford University
K. Belczynski, Northwestern University
R. Bennett, University of Glasgow
S. J. Berukoff, Max Planck Institute for Gravitational Physics (Albert Einstein Institute)
J. Betzwieser, Massachusetts Institute of Technology
B. Bhawal, California Institute of Technology
I. A. Bilenko, Lomonosov Moscow State University
G. Billingsley, California Institute of Technology
E. Black, California Institute of Technology

Document Type

Article

Publication Date

5-13-2005

Abstract

We place direct upper limits on the amplitude of gravitational waves from 28 isolated radio pulsars by a coherent multidetector analysis of the data collected during the second science run of the LIGO interferometric detectors. These are the first direct upper limits for 26 of the 28 pulsars. We use coordinated radio observations for the first time to build radio-guided phase templates for the expected gravitational-wave signals. The unprecedented sensitivity of the detectors allows us to set strain upper limits as low as a few times 10-24. These strain limits translate into limits on the equatorial ellipticities of the pulsars, which are smaller than 10-5 for the four closest pulsars. © 2005 The American Physical Society.

Publication Source (Journal or Book title)

Physical Review Letters

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