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Czechoslovak Journal of Physics

Diamagnetism of a gas of 2D-fermions in strong non-homogeneous magnetic fields and anyons

O. Hudák

Published Jan 1, 1994• 0 citations
Publisher
DOI
10.1007/bf01691749

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Diamagnetism of 2D-Fermions in the Strong Nonhomogeneous Static Magnetic Field (B=B(0,0,1/cosh2(x−x0δ)))( {\bf B} =B( 0, 0, 1/cosh^{2}( \frac{x-x_{0} }{ δ})))(B=B(0,0,1/cosh2(δx−x0​​))) : gas magnetization, ... and gas compressibility
We study diamagnetism of a gas of fermions moving in a nonhomogeneous magnetic field (B=B(0,0,1/cosh2(x−x0δ)))( {\bf B} =B( 0, 0, 1/cosh^{2}( \frac{x-x_{0} }{ δ})))(B=B(0,0,1/cosh2(δx−x0​​))) The gas magnetization, the static magnetic susceptibility, the chemical potential and the gas compressibility are discussed and compared with the uniform field case. General need to study dynamics of electrons in different types of magnetic fields follows from a large number of experimental situations in which its understanding enables physicists to obtain new information.
We present analytic formulas for the ground state energy of two-dimensional (2D) anyon gas in strong magnetic field (Landau level filling factor νL ≤ 1). The formulas are obtained by applying harmonic potential regularization for the vanishing confinement to harmonically confined Coulomb anyon gas. In a case of absence of the Coulomb interaction our analytic result provides an exact solution. It contains a contribution of the anyon gauge field characterized by the anyon parameters ν and νL. In a case of presence of the Coulomb interaction we introduce a function depending on the parameters ν, νL and the density parameter rs. The function is determined by fitting the Fano-Ortolani interpolation equation in the fractional quantum Hall effect regime for spin-polarized electrons and by consistence requirement with known results for the ground state energy of the 2D Coulomb Bose gas in strong magnetic field. We show that our formulas are valid not only for fermions (ν=1) but quite generally for anyons (0 ≤ ν ≤ 1).