- Access by Xinjiang University
Cumulative analysis of the association between the data of the gravitational wave detectors NAUTILUS and EXPLORER and the gamma ray bursts detected by BATSE and BeppoSAX
Phys. Rev. D 71, 042001 – Published 14 February, 2005
DOI: https://doi.org/10.1103/PhysRevD.71.042001
Abstract
The statistical association between the output of the Gravitational Wave (GW) detectors EXPLORER and NAUTILUS and a list of Gamma Ray Bursts (GRBs) detected by the satellite experiments BATSE and BeppoSAX has been analyzed using cumulative algorithms. GW detector data collected between 1991 and 1999 have been searched for an energy excess in a 10 s interval around the GRB flux peak times. The cumulative analysis of the data relative to a large number of GRBs (387) allows to push the upper bound for the corresponding GW burst amplitude down to .
Article Text
References (33)
- G. J. Fishman and C. A. Meegan, Annu. Rev. Astron. Astrophys. 33, 415 (1995).
- M. S. Briggs et al., Astrophys. J. 459, 40 (1996).
- G. Boella et al., Astron. Astrophys. Suppl. Ser. 122, 299 (1997).
- E. Costa et al., Nature (London) 387, 783 (1997).
- W. S. Paciesas et al., Astrophys. J. Suppl. Ser. 122, 465 (1999).
- C. Guidorzi et al., in Gamma-Ray Bursts in the Afterglow Era, edited by E. Costa, F. Frontera, and J. Hjorth (Springer-Verlag, Berlin, 2001), p. 43.
- http://gammaray.msfc.nasa.gov/batse/grb/catalog/
- L. S. Finn, S. D. Mohanty, and J. D. Romano, Phys. Rev. D 60, 121101 (1999).
- G. Modestino and G. Pizzella, Astron. Astrophys. 364, 419 (2000).
- M. T. Murphy, J. K. Webb, and I. S. Heng, Mon. Not. R. Astron. Soc. 316, 657 (2000).
- P. Bonifazi et al., Astronomical and Astrophysical Transactions 22, 557 (2003).
- G. Modestino and A. Moleti, Phys. Rev. D 65, 022005 (2002).
- P. Astone et al., Phys. Rev. D 66, 102002 (2002).
- M. J. Rees and P. Mészáros, Astrophys. J., Lett. Ed. 430, L93 (1994).
- T. Piran, Phys. Rep. 314, 575 (1999).
- P. Mészáros, Science 291, 79 (2001).
- B. Zhang and P. Mészáros, Int. J. Mod. Phys. A 19, 2385 (2004).
- A. De Rujúla, astro-ph/0207033.
- S. Kobayashi and P. Mészáros, Astrophys. J. 589, 861 (2003).
- M. H. P. M. van Putten, Phys. Rep. 345, 1 (2001); M. H. P. M. van Putten et al., Phys. Rev. D 69, 044007 (2004).
- F. Frontera et al., Astrophys. J. Suppl. Ser. 127, 59 (2000).
- F. Frontera, Lecture Notes in Physics, (Springer, Berlin, Heidelberg, 2003), edited by K. W. Weiler vol. 598, p. 317.
- R. Sari, T. Piran, and R. Narayan, Astrophys. J., Lett. Ed. 497, L17 (1998).
- G. Modestino et al., in Proceedings of Gravitational Wave Data Analysis Workshop 2, Orsay, 1997, edited by M. Davier and P. Hello, p. 187.
- G. Modestino et al., in Proceedings of Frontier Objects in Astrophysics and Particle Physics, Vulcano, 1998, edited by F. Giovannelli and G. Mannocchi, p. 295.
- P. Tricarico et al., Phys. Rev. D 63, 082002 (2001).
- P. Astone et al., Classical Quantum Gravity 19, 5449 (2002).
- S. D. Márka, talk given at Gravitational Wave Data Analysis Workshop 8, Milwaukee, Wisconsin, 2003 (unpublished).
- A preliminary analysis of these data was presented at the 2003 Amaldi conference: P. Astone et al., Classical Quantum Gravity 21, S759 (2004).
- P. Astone, P. Bonifazi, G. V. Pallottino, and G. Pizzella, Nuovo Cimento Soc. Ital. Fis. C 17, 713 (1994).
- W. T. Eadie, D. Drijard, F. L. James, and B. Saudoulet, Statistical Method in Experimental Physics (North-Holland Publishing Company, Amsterdam, 1971).
The choice of 10 s as integration interval comes from estimating the possible differences between the true GRB arrival time and the flux peak time, and from the time resolution of our data. In principle, the optimal choice is to have an integration interval of the same order of the overall time uncertainty. This choice will imply losing sensitivity when the GW detector decay time is smaller than 10 s, which occurs about of the times.
- G. D’Agostini, Bayesian Reasoning in Data analysis (World Scientific, Singapore, 2003).