Langevin equation (overdamped):
dx/dt = −V'(x)/γ + √(2kT/γ) η(t)
V(x) = a·x⁴ − 2a·x² (double well, minima at x=±1, barrier at x=0 height a).
Kramers escape rate:
Γ = (ω₀ω_b)/(2πγ) exp(−ΔV/kT)
where ΔV = a, ω₀²=|V''(±1)|=4a, ω_b²=|V''(0)|=4a.
The histogram converges to the Boltzmann distribution P(x) ∝ e^{−V(x)/kT}.