Abstract
Valence band ( hh and lh) states in B δ-doped diamond quantum wells are calculated within the effective mass approximation using a local density Thomas-Fermi approximation for the description of the band bending profile. Many-body Hartree, exchange and correlation terms are included in the potential energy well function. The diagonalization of the Kohn–Luttinger Hamiltonian is performed using different sets of Luttinger parameters for diamond reported in the literature. The results could be useful in identifying the actual valence band structure of diamond.
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