Abstract

The dynamical properties of the impurity pinning of phasons of the charge-density wave are investigated for two-dimensional electron systems in the presence of magnetic fields applied perpendicular to the system. The effect of magnetic fields is treated classically. It is found that there exists a finite size of domains if the impurity potential overwhelms the long-range part of mutual Coulomb interactions, and the magnetoconductivity tensor is evaluated in such cases. The cyclotron resonance is shown to be shifted and broadened. It is predicted that absorption of electromagnetic waves exists at the pinned-mode frequency though the oscillator strength will be smaller by a factor of ${({\ensuremath{\omega}}_{c}\ensuremath{\tau})}^{\ensuremath{-}2}$ than the cyclotron resonance if ${\ensuremath{\omega}}_{c}\ensuremath{\tau}\ensuremath{\gg}1$, where ${\ensuremath{\omega}}_{c}$ and $\ensuremath{\tau}$ are the cyclotron frequency and the damping of the resonance, respectively.

Keywords

PhysicsCondensed matter physicsCyclotron resonanceOmegaCyclotronMagnetic fieldImpurityCoulombElectronResonance (particle physics)Atomic physicsQuantum mechanics

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Publication Info

Year
1978
Type
article
Volume
18
Issue
11
Pages
6245-6252
Citations
149
Access
Closed

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Hidetoshi Fukuyama, Patrick A. Lee (1978). Pinning and conductivity of two-dimensional charge-density waves in magnetic fields. Physical review. B, Condensed matter , 18 (11) , 6245-6252. https://doi.org/10.1103/physrevb.18.6245

Identifiers

DOI
10.1103/physrevb.18.6245