D = 0.20
ΔV = 0.30
ε = 0.00
Current x—
Well (+)—
Well (−)—
Transitions—
Kramers rate—
SDE: dx = −V′(x)dt + √(2D)dW. Kramers rate: k ≈ (ω₀ω_b/2π)e^(−ΔV/D). Low D: particle trapped. High D: frequent transitions. Asymmetry biases occupation. Noise-induced transitions can create qualitatively new stable states.