Derives universal relation ρ_c ∼ λ_D √(ℓ/L) for coherence length in Coulomb-disordered media using Efimov path-integral formalism, linking it to single-particle localization length ℓ.
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Extends static disorder-induced localization of a quantum particle in a classical one-component plasma to the dynamic regime, deriving a velocity-dependent effective disorder strength that alters localization scaling for slow particles.
Derives closed-form expressions for the localization length of a quantum particle in a classical plasma, incorporating the Coulomb logarithm ln(κ L) in both weak- and strong-disorder regimes via path-integral methods.
citing papers explorer
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Localization of a quantum particle in a classical one-component plasma.III. Mutual coherence and coherence degradation in Coulomb-disordered media
Derives universal relation ρ_c ∼ λ_D √(ℓ/L) for coherence length in Coulomb-disordered media using Efimov path-integral formalism, linking it to single-particle localization length ℓ.
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Localization of a quantum particle in a classical one-component plasma. II. Dynamic Disorder and Temporal Decorrelation
Extends static disorder-induced localization of a quantum particle in a classical one-component plasma to the dynamic regime, deriving a velocity-dependent effective disorder strength that alters localization scaling for slow particles.
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Localization of a quantum particle in a classical one-component plasma. Fluctuation-induced random potential and the Coulomb logarithm
Derives closed-form expressions for the localization length of a quantum particle in a classical plasma, incorporating the Coulomb logarithm ln(κ L) in both weak- and strong-disorder regimes via path-integral methods.