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[40]) we can decompose any arbitraryn N ×n N matrix in terms of them: O= 1 nN Tr(O) + 1 nN−1 2 Tr OΛAa ΛAa +

Operator Decomposition, Completeness, Operator Transformations, Operator Action Since all possible products of Λ AµA ’s are Hermitian matrices of the fundamental representati

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Improved Approximations for Collective Neutrino Oscillations

hep-ph · 2026-07-30 · conditional · novelty 5.0

A second-order BBGKY closure reproduces exact small-system neutrino dynamics about two orders of magnitude better than mean-field at polynomial cost, and predicts correlated large-N behavior.

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  • Improved Approximations for Collective Neutrino Oscillations hep-ph · 2026-07-30 · conditional · none · ref 1

    A second-order BBGKY closure reproduces exact small-system neutrino dynamics about two orders of magnitude better than mean-field at polynomial cost, and predicts correlated large-N behavior.