Authors

G. M. Harry, Massachusetts Institute of Technology
R. Adhikari, Massachusetts Institute of Technology
S. Ballmer, Massachusetts Institute of Technology
K. Bayer, Massachusetts Institute of Technology
J. Betzwieser, Massachusetts Institute of Technology
B. Bochner, Massachusetts Institute of Technology
R. Burgess, Massachusetts Institute of Technology
L. Cadonati, Massachusetts Institute of Technology
S. Chatterji, Massachusetts Institute of Technology
T. Corbitt, Massachusetts Institute of Technology
P. Csatorday, Massachusetts Institute of Technology
P. Fritschel, Massachusetts Institute of Technology
K. Goda, Massachusetts Institute of Technology
Y. Hefetz, Massachusetts Institute of Technology
E. Katsavounidis, Massachusetts Institute of Technology
R. Lawrence, Massachusetts Institute of Technology
M. Macinnis, Massachusetts Institute of Technology
A. Marin, Massachusetts Institute of Technology
K. Mason, Massachusetts Institute of Technology
N. Mavalvala, Massachusetts Institute of Technology
R. Mittleman, Massachusetts Institute of Technology
D. J. Ottaway, Massachusetts Institute of Technology
M. Pratt, Massachusetts Institute of Technology
T. Regimbau, Massachusetts Institute of Technology
S. Richman, Massachusetts Institute of Technology
J. Rollins, Massachusetts Institute of Technology
D. H. Shoemaker, Massachusetts Institute of Technology
M. Smith, Massachusetts Institute of Technology
M. Van Putten, Massachusetts Institute of Technology
R. Weiss, Massachusetts Institute of Technology
C. Aulbert, Max Planck Institute for Gravitational Physics (Albert Einstein Institute)
S. J. Berukoff, Max Planck Institute for Gravitational Physics (Albert Einstein Institute)
C. Cutler, Max Planck Institute for Gravitational Physics (Albert Einstein Institute)

Document Type

Article

Publication Date

1-1-2006

Abstract

The LIGO interferometers are operating as gravitational wave observatories, with a noise level near an order of magnitude of the goal and the first scientific data recently taken. This data has been analyzed for four different categories of gravitational wave sources; millisecond bursts, inspiralling binary neutron stars, periodic waves from a known pulsar, and stochastic background. Research and development is also underway for the next generation LIGO detector, Advanced LIGO.

Publication Source (Journal or Book title)

The Tenth Marcel Grossmann Meeting: On Recent Developments in Theoretical and Experimental General Relativity, Gravitation and Relativistic Field Theories

First Page

308

Last Page

336

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