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- W3023946421 abstract "This chapter gives a thermodynamic overview of an ideal Fermi gas. The fugacity of the gas in the Fermi case can take on unrestricted values ranging from zero to infinity. Moreover, in view of the Pauli exclusion principle, the question of a large number of particles occupying a single energy state does not even arise in this case, because of which there is no phenomenon like Bose–Einstein condensation in an ideal Fermi gas. Nevertheless, at sufficiently low temperatures, Fermi gas displays its own brand of quantal behavior. In quantum statistics, an effect that is totally absent in classical statistics is diamagnetic in character and arises from the quantization of the orbits of charged particles in the presence of an external magnetic field or from the quantization of the energy of charged particles associated with their motion perpendicular to the direction of the field. The equilibrium state of a gas of non-interacting fermions in the presence of an external magnetic field is calculated by determining the net magnetic moment acquired by the gas and then calculating its susceptibility. In general, the magnetic behavior of a Fermi gas is determined jointly by the intrinsic magnetic moment of the particles and the quantization of their orbits. If the spin-orbit interaction is negligible, the resultant behavior is obtained by a simple addition of the two effects. The chapter also gives a brief account of the phenomena of thermionic and photoelectric emission of electrons from metals and examines the influence of a moderately strong electric field on the thermionic emission from a metal." @default.
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- W3023946421 date "1996-01-01" @default.
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- W3023946421 title "IDEAL FERMI SYSTEMS" @default.
- W3023946421 doi "https://doi.org/10.1016/b978-075062469-5/50010-4" @default.
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