Extends classical nucleation theory to nonequilibrium non-conserved scalar fields by showing the time-reversed-relaxation ansatz fails and deriving corrected quasipotentials via two independent routes, validated numerically.
As we haveL †ψ′ =L † λ∗,h∗ ψ′ +O(δλ, δh), we conclude that cφ′ 0e−2λ∗φ0/K +O(δλ, δh)∈Ker(L †).(39) Herecis a constant that cancels in the following and can thus be set to unity
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Nucleation and time-reversal symmetry breaking in nonconserved scalar field theories
Extends classical nucleation theory to nonequilibrium non-conserved scalar fields by showing the time-reversed-relaxation ansatz fails and deriving corrected quasipotentials via two independent routes, validated numerically.