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Ultrarelativistic magnetic monopole search with the ANITA-II balloon-borne radio interferometer
Phys. Rev. D 83, 023513 – Published 19 January, 2011
DOI: https://doi.org/10.1103/PhysRevD.83.023513
Abstract
We have conducted a search for extended energy deposition trails left by ultrarelativistic magnetic monopoles interacting in Antarctic ice. The nonobservation of any satisfactory candidates in the 31 days of accumulated ANITA-II (Antarctic Impulsive Transient Antenna) flight data results in an upper limit on the diffuse flux of relativistic monopoles. We obtain a 90% C.L. limit of order for values of Lorentz factor, , at the anticipated energy . This bound is stronger than all previously published experimental limits for this kinematic range.
Article Text
References (32)
- J. C. Clerk, Phil. Trans. R. Soc. London 155, 459 (1865).
- A. H. Guth, Phys. Rev. D 23, 347 (1981).
- P. A. M. Dirac, Proc. R. Soc. A 133, 60 (1931).
- P. B. Price, E. K. Shirk, W. Z. Osborne, and L. S. Pinsky, Phys. Rev. Lett. 35, 487 (1975).
- B. Cabrera, Phys. Rev. Lett. 48, 1378 (1982).
- A. D. Caplin, M. Hardiman, M. Koratzinos, and J. C. Schouten, Nature (London) 321, 402 (1986).
- P. B. Price, E. K. Shirk, W. Z. Osborne, and L. S. Pinsky, Phys. Rev. D 18, 1382 (1978).
- M. E. Huber, B. Cabrera, M. A. Taber, and R. D. Gardner, Phys. Rev. Lett. 64, 835 (1990).
- E. N. Parker, Astrophys. J. 160, 383 (1970).
- M. Ambrosio et al. (MACRO Collaboration), Eur. Phys. J. C 25, 511 (2002).
- H. Wissing for the (IceCube Collaboration) in Proceedings of the 30th International Cosmic Ray Conference (ICRC), Merida, Mexico, 2007 (unpublished).
- V. Aynutdinov et al. (Baikal Collaboration), in Proceedings of the 29th International Cosmic Ray Conference (ICRC), Pune, India, 2005 (unpublished).
The flux limit from Baikal assumes an initial monopole energy of , lower than the initial energy assumed in this study. Therefore, the Baikal limit shown in Fig. 12 should be regarded as a function of the indicated mass but not necessarily the indicated .
- S. Balestra et al. (SLIM Collaboration), Eur. Phys. J. C 55, 57 (2008).
- F. C. Adams, M. Fatuzzo, K. Freese, G. Tarlé, R. Watkins, and M. S. Turner, Phys. Rev. Lett. 70, 2511 (1993); astrophysical limits tabulated in [32].
- S. D. Wick, T. W. Kephart, T. J. Weiler, and P. L. Biermann, Astropart. Phys. 18, 663 (2003).
- J. D. Jackson, Classical Electrodynamics (Wiley, New York, 1962).
- D. P. Hogan et al., Phys. Rev. D 78, 075031 (2008).
- P. W. Gorham et al. (ANITA Collaboration), Astropart. Phys. 32, 10 (2009).
- P. W. Gorham et al. (ANITA Collaboration), Phys. Rev. Lett. 103, 051103 (2009).
- P. W. Gorham et al. (ANITA Collaboration), Phys. Rev. D 82, 022004 (2010), and erratum arXiv:1011.5004.
- S. Hoover et al. Phys. Rev. Lett. 105, 151101 (2010),
- S. Iyer Dutta, M. H. Reno, I. Sarcevic, and D. Seckel, Phys. Rev. D 63, 094020 (2001); D. Seckel, M. H. Reno, I. Sarkevic, and S. Iyer Dutta, in Proceedings of the 27th International Cosmic Ray Conference (ICRC), Hamburg, Germany, 2001 (unpublished).
The loss symbol should cause no confusion with the velocity .
- L. D. Landau and I. J. Pomeranchuk, Dokl. Akad. Nauk SSSR 92, 535 (1953); 92, 735 (1953); A. B. Migdal, Phys. Rev. 103, 1811 (1956); J. Alvarez-Muñiz, R. A. Vázquez and E. Zas, Phys. Rev. D 61, 023001 (1999).
- A. M. Dziewonski and D. L. Anderson, Phys. Earth Planet. Inter. 25, 297 (1981).
- I. Kravchenko et al. (RICE Collaboration), Phys. Rev. D 73, 082002 (2006).
- D. Saltzberg et al., Phys. Rev. Lett. 86, 2802 (2001).
- P. Gorham et al.Phys. Rev. D 72, 023002 (2005).
- R. V. Buniy and J. P. Ralston, Phys. Rev. D 65, 016003 (2001).
- D. Chirkin and W. Rhode, arXiv:hep-ph/0407075
- C. Amsler et al. (Particle Data Group), Phys. Lett. B 667, 1 (2008).