(B32), this becomes 0= d dt [GAB ˙Y B+ AA I (Q−AC ˙Y C)]−1 2 ∂AGBC ˙Y B ˙Y C+∂ AU +1 2 ∂A( 1 I)(Q−A C ˙Y C) 2 −1 I(Q−AC ˙Y C)∂ AAB ˙Y B ,(B35) where∂ A ≡δ/δY A

Equations of motion at fixed charge The reduced action is SR[Y, Q]= ∫ ∆t 0 dt R(Y, ˙Y, Q)

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hep-th · 2026-04-09 · unverdicted · novelty 7.0

A first-principles Euclidean prescription for tunnelling rates out of Noether-charged states, including cases with non-trivial energy.

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On quantum tunnelling in the presence of Noether charges hep-th · 2026-04-09 · unverdicted · none · ref 21
A first-principles Euclidean prescription for tunnelling rates out of Noether-charged states, including cases with non-trivial energy.