Abstract
The energy of the bottom of the conduction zone and the effective mass of excess electrons injected into a nonpolar fluid with high polarizability is considered. Pseudopotential theory of electrons in a cellular medium is extended to conditions where polarization attraction predominates over electron-fluid interaction. The solution is obtained in the Wigner-Seitz cell for the case where the scattering length of electron in the fluid is negative. The calculated density dependences of the conduction-zone bottom and effective mass of electron in noble fluids are in satisfactory agreement with available experimental data.
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