Abstract
The overall hardness scale of the ultra-high energy neutrino-nucleon interactions is usually estimated as Q 2 ∼ m 2 w The effect of non-conservation of weak currents pushes this scale up to the top quark mass squared and changes dynamics of the scattering process. The Double Leading Log Approximation provides simple and numerically accurate formula for the top-bottom contribution to the total cross section σνN. Corresponding correction to σνN appears to be numerically large. It is comparable with the leading contribution evaluated in the massless quark approximation.
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References
J. K. Becker, Phys. Rep. 458, 173 (2008).
G. M. Frichter, D. W. McKay, and J. P. Ralston, Phys. Rev. Lett. 74, 1508 (1995); Phys. Rev. Lett. 77, 4107(E) (1996); R. Gandhi, C. Quigg, M. H. Reno, and I. Sarcevic, Astropart. Phys. 5, 81 (1996); Phys. Rev. D 58, 093009 (1998); G. Parente and E. Zas, in Proceedings of the 7th International Symposium on Neutrino Telescopes, Venice, Italy, Feb. 1996, p. 499, astroph/9606091; G. C. Hill, Astropart. Phys. 6, 215 (1997); M. V. T. Machado, Phys. Rev. D 70, 053008 (2004); R. Fiore, L. L. Jenkovszky, A. V. Kotikov, et al., Phys. Rev. D 73, 053012 (2006).
M. Glück, S. Kretzer, and E. Reya, Astropart. Phys. 11, 327 (1999); J. Kwiecinski, A. D. Martin, and A. M. Stasto, Phys. Rev. D 59, 093002 (1999); Y. S. Jeong and M. H. Reno, Phys. Rev. D 81, 114012 (2010); M. Glück, P. Jimenez-Delgado, and E. Reya, Phys. Rev. D 81, 097501 (2010).
E. M. Henley and J. Jalilian-Marian, Phys. Rev. D 73, 094004 (2006).
K. Kutak and J. Kwiecinski, Eur. Phys. J. C 29, 521 (2003).
R. Fiore and V. R. Zoller, Saturation Talk at Diffraction 2010, Otranto (Lecce), Italy, September 10–15, 2010.
V. Barone, M. Genovese, N. N. Nikolaev, et al., Phys. Lett. B 328, 143 (1994).
R. Fiore and V. R. Zoller, JETP Lett. 87, 524 (2008); in Proceedings of the 43rd Rencontres de Moriond on QCD and Hadronic Interactions, 2008 QCD and High Energy Interactions, La Thuile, Italy, 2008, e-Print: arXiv:0805.2090.
R. Fiore and V. R. Zoller, Phys. Lett. B 681, 32 (2009); AIP Conf. Proc. 1105, 304 (2009).
V. N. Gribov and L. N. Lipatov, Sov. J. Nucl. Phys. 15, 438 (1972); L. N. Lipatov, Sov. J. Nucl. Phys. 20, 181 (1974); Yu. L. Dkshitzer, Sov. Phys. JETP 46, 641 (1977); G. Altarelli and G. Parisi, Nucl. Phys. B 126, 298 (1977); R. G. Roberts, The Structure of the Proton (Cambridge Univ., Cambridge, 1990).
I. P. Ivanov and N. N. Nikolaev, Phys. Rev. D 65, 054004 (2003).
M. Glück, E. Reya, and A. Vogt, Eur. Phys. J. C 5, 461 (1998).
O. V. Kancheli, Sov. Phys. JETP Lett 18, 274 (1973).
N. N. Nikolaev and V. I. Zakharov, Phys. Lett. B 55, 397 (1975); Sov. J. Nucl. Phys. 21, 227 (1975).
L. V. Gribov, E. M. Levin, and M. G. Ryskin, Phys. Rep. 100, 1 (1981); A. H. Mueller and J. Qiu, Nucl. Phys. B 268, 427 (1986).
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Fiore, R., Zoller, V.R. Current non-conservation effects in ultra-high energy neutrino interactions. Jetp Lett. 92, 654–657 (2010). https://doi.org/10.1134/S0021364010220030
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DOI: https://doi.org/10.1134/S0021364010220030