Proc. Neutrino Astrophysics - MPP Theory Group
Proc. Neutrino Astrophysics - MPP Theory Group
Proc. Neutrino Astrophysics - MPP Theory Group
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Today, however, charm production experiments give a consistent set of data, and are compatible<br />
with QCD calculations to next-to-leading order [11]. This has removed the impetus<br />
to look for unconventional mechanisms of charm production, and has motivated a detailed<br />
study of atmospheric neutrinos within perturbative QCD [12].<br />
In Fig. 1 I have collected some of the expected astrophysical neutrino signals and several<br />
predictions for the high energy atmospheric background. The astrophysical signals shown<br />
are the diffuse fluxes from blazars estimated by Dar and Shaviv [13], Protheroe [14], and<br />
Mannheim [15], and the neutrino emission from the galactic interstellar medium as calculated<br />
by Domokos et al. [16]. The conventional atmospheric background is from Lipari [17], and<br />
the prompt neutrino fluxes are from Zas et al. (ZHVa for model A, ZHVe for model E) [4],<br />
Volkova et al. (VFGS) [9], Bugaev et al. (BNSZ) [10], Gonzalez-Garcia et al. (GGHVZ) [7],<br />
and Thunman et al. (TIG) [12]. Also indicated are the upper limits on the prompt neutrino<br />
flux from MACRO [18] and AKENO [19]. Although these limits exclude the highest prediction<br />
ZHVa, the remaining uncertainty in the prompt neutrino background is still a factor of 100.<br />
Since the high-energy atmospheric neutrino background may be a nuisance to the detection<br />
of astrophysical diffuse neutrino fluxes, it may be of value to decrease the uncertainty in the<br />
predictions. The best way would be a detection of the associated prompt muons, maybe<br />
through larger air shower arrays. A second option would be to increase the precision of the<br />
theoretical inputs, for example through better measurement of the charm production cross<br />
section and the charm semileptonic decay rates, which is under way/under project in high<br />
statistics charm production experiments. At last, it may happen that we have to wait for the<br />
neutrino telescopes themselves to know the high energy atmospheric neutrino background.<br />
References<br />
[1] See discussion in M. Ambrosio et al., Phys. Rev. D52 (1995) 3793.<br />
[2] A. Kernan and G. Van Dalen, Phys. Rep. 106 (1984) 297; S.P.K. Tavernier, Rep. Prog.<br />
Phys. 50 (1987) 1439.<br />
[3] H. Inazawa and K. Kobayakawa, Prog. Theor. Phys. 60 (1983) 1195.<br />
[4] E. Zas, F. Halzen, R.A. Vázques, Astropart. Phys. 1 (1993) 297.<br />
[5] L.V. Volkova, Yad. Fiz. 31 (1980) 1510 [Sov. J. Nucl. Phys. 31 (1980) 784].<br />
[6] C. Castagnoli et al., Nuovo Cimento A82 (1984) 78.<br />
[7] M.C. Gonzalez-Garcia et al., Phys. Rev. D49 (1994) 2310.<br />
[8] G. Battistoni et al., Astropart. Phys. 4 (1996) 351.<br />
[9] L.V. Volkova et al., Nuovo Cimento C10 (1987) 465.<br />
[10] E.V. Bugaev et al., Nuovo Cimento C12 (1989) 41.<br />
[11] J.A. Appel, Ann. Rev. Nucl. part. Sci. 42 (1992) 367; S. Frixione et al., in Heavy Flavours<br />
II, eds. A.J. Buras and M. Lindner (World Scientific), hep-ph/9702287; G.A. Alves et<br />
al., Phys. Rev. Lett. 77 (1996) 2388.<br />
[12] M. Thunman, G. Ingelman, P. Gondolo, Astropart. Phys. 5 (1996) 309.