Electrons in a periodic lattice under DC field — semiclassical transport theory
Band Structure E(k) & Electron Motion
Velocity v(k) & Current
Real-space position x(t)
Esaki-Tsu J(E) curve
Phase space (k,x)
Physics: In a periodic lattice, electrons undergo Bloch oscillations with frequency
ω_B = eEa/ℏ. The Esaki-Tsu formula gives current
J ∝ E·τ/(1+(ω_B·τ)²) — peak at ω_B·τ = 1, then negative differential resistance (NDR) for stronger fields.
NDR period: — | ω_B·τ = — | Regime: —