mesoscopic-physics

Layer 1 — Physics24 concepts in this subtree

Quantum-coherent transport in conductors whose linear dimensions are smaller than the phase-coherence length L_φ but larger than the elastic mean free path ℓ — i.e. the regime where the wave nature of electrons matters macroscopically yet…

Landauer-Büttiker formula: G = (2e²/h)·Σ T_n
Aharonov-Bohm effect: gauge-invariant phase, period Φ_0 = h/e
Wiedemann-Franz law: κ/(σT) = π²k_B²/(3e²)
Landauer: N open modes give G = N·G_0 exactly
AB period Φ_0 = h/e, phase-per-period = 2π (exact)
Lorenz number L_0·e²/k_B² = π²/3 (exact rational π²)
Kondo one-loop RG: scaling equation dJ/d ln(Lambda) = -rho J^2; dynamical scale T_K = Lambda_0 exp(-1/(2 rho J_0))
UCF conductance variance identity: det(A A^T) = sum_{|S|=m} det(A_S)^2 (Cauchy-Binet)
Aharonov-Bohm periodicity: current I(Phi) has period Phi_0 = h/e (U(1) covering space of annulus)
Theorem: Kondo dynamical scale T_K = Lambda_0 * exp(-1/(2 rho J_0)) (RG integration)
Theorem: Cauchy-Binet residual det(A A^T) - sum det(A_S)^2 = 0 (2x3 UCF test matrix)
Theorem: AB periodicity I(Phi + Phi_0) - I(Phi) = 0 for I(Phi) = cos(2 pi Phi / Phi_0)
Aharonov-Bohm (1959)
Landauer-Buttiker (1985)
Kondo effect (1964)
Quantum Hall (Klitzing 1980)
FQHE (Tsui-Stormer 1982)
UCF (Altshuler 1985)
Landauer (1957)
Büttiker (1986)
Aharonov-Bohm (1959)
QPC (van Wees 1988)
Coulomb blockade (Fulton-Dolan 1987)
RMT (Mehta 1960)
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