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Detecting the Gravitational Wave background using Millisecond Pulsars Fredrick A. Jenet Center for Gravitational Wave Astronomy University of Texas at.

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Presentation on theme: "Detecting the Gravitational Wave background using Millisecond Pulsars Fredrick A. Jenet Center for Gravitational Wave Astronomy University of Texas at."— Presentation transcript:

1 Detecting the Gravitational Wave background using Millisecond Pulsars Fredrick A. Jenet Center for Gravitational Wave Astronomy University of Texas at Brownsville

2 Collaborators Dick Manchester ATNF/CSIRO Australia George Hobbs ATNF/CSIRO Australia KJ Lee Peking U. China Andrea Lommen Franklin & Marshall USA Shane L. Larson Penn State USA Linqing Wen AEI Germany Teviet Creighton Caltech USA John Armstrong JPL USA

3 What can we do with an array of pulsars and the G-wave background? 1.Make a definitive detection of G-waves. 2.Measure the polarization properties of G-waves. 3.Place limits on the graviton mass. 4.Study the properties of the G- wave source.

4 The most likely source of G-waves will be a stochastic background generated by super-massive binary black holes distributed throughout the universe! Jaffe & Backer (2002) Wyithe & Lobe (2002) Enoki, Inoue, Nagashima, Sugiyama (2004) Like the cosmic micro-wave background, the G-wave background is an incoherent sum of G-waves. h c = A f -   = 2/3 A = 10 -15 to 10 -14 yrs -2/3

5 Detecting G-waves The presence of G-waves will cause the rate of arrival a individual pulses to fluctuate.

6 kk  Photon Path G-wave Pulsar Earth

7 Important Points

8 The timing residuals for a stochastic background This is the same for all pulsars. This depends on the pulsar. The induced residuals for different pulsars will be correlated.

9 Two-point correlation Two basic techniques Spherical Harmonic Decomposition Hellings & Downs 1983 Jenet, Hobbs, Lee, & Manchester 2005 Hellings 1990 Jaffe & Backer 2002

10 Single Pulsar Limit (1  s, 7 years) Expected Regime For a background of SMBH binaries: h c = A f -2/3

11 Single Pulsar Limit (1  s, 7 years) 1  s, 1 year (Current ability) Expected Regime For a background of SMBH binaries: h c = A f -2/3

12 Single Pulsar Limit (1  s, 7 years) 1  s, 1 year (Current ability) Expected Regime.1  s 5 years For a background of SMBH binaries: h c = A f -2/3

13 Single Pulsar Limit (1  s, 7 years) 1  s, 1 year (Current ability) Expected Regime.1  s 5 years.1  s 10 years For a background of SMBH binaries: h c = A f -2/3

14 Single Pulsar Limit (1  s, 7 years) 1  s, 1 year (Current ability) Expected Regime.1  s 5 years.1  s 10 years SKA 10 ns 5 years 40 pulsars For a background of SMBH binaries: h c = A f -2/3

15 Single Pulsar Limit (20 ns, 2 years) 1  s, 1 year (Current ability) Expected Regime.1  s 5 years.1  s 10 years SKA 10 ns 5 years 40 pulsars For a background of SMBH binaries: h c = A f -2/3

16 G-wave polarization properties

17 Graviton Mass Current solar system limits place m g < 4.4 10 - 22 eV  2 = k 2 + (2  m g /h) 2 < 1/ (4 months) Detecting 5 year period G-wave reduces the upper bound of the graviton mass by a factor of 15.


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