Non-standard in tf rac tj ons in atmospheric neu ts ino experiments Arman Esmaili Pontifícia Universidade Católica do Rio de Janeiro (PUC-Rio), Brasil
<latexit sha1_base64="bc+RhuwbF6Cwklh4tdZExbSpzhI=">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</latexit> <latexit sha1_base64="bc+RhuwbF6Cwklh4tdZExbSpzhI=">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</latexit> <latexit sha1_base64="bc+RhuwbF6Cwklh4tdZExbSpzhI=">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</latexit> Standard high energy atm oscillation ✔ The standard oscillation of neutrinos disappear with the increase of energy For ν e (although the osc. length converges to the refraction length ~ Earth’s radius): 1 sin 2 2 θ m ∝ 2 G F E ν n e ) 2 → 0 √ (2 For ν µ and ν τ the mixing angle is unsuppressed, but the osc. length increases with energy and becomes much larger than the Earth’s diameter. For energies >~ 100 GeV, no standard oscillation Arman Esmaili PANE 2018 @ ICTP 29/May/2018
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