We compute within the effective-mass theory and without adjustable parameters the Stark effect for shallow P donors in Si with anisotropic band structure. Valley-orbit coupling is taken into account in a nonperturbative way and scattering effects of the impurity core are included to properly describe low-lying impurity states. The ground-state energy slightly decreases with increasing electric field up to a critical value E-cr similar to 25 keV/cm, at which the donor can be ionized by tunneling due to a field-induced mixing of the '1s-like' singlet ground state with a '2p(0)-like' excited state in zero field. The resulting ground-state wave function at high field extends significantly outside the potential barrier surrounding the impurity. Calculations of the hyperfine splitting and of the A-shell superhyperfine coupling constants as a function of the electric field complete the work.

Computation of the Stark effect in P impurity states in silicon

Debernardi A;
2006

Abstract

We compute within the effective-mass theory and without adjustable parameters the Stark effect for shallow P donors in Si with anisotropic band structure. Valley-orbit coupling is taken into account in a nonperturbative way and scattering effects of the impurity core are included to properly describe low-lying impurity states. The ground-state energy slightly decreases with increasing electric field up to a critical value E-cr similar to 25 keV/cm, at which the donor can be ionized by tunneling due to a field-induced mixing of the '1s-like' singlet ground state with a '2p(0)-like' excited state in zero field. The resulting ground-state wave function at high field extends significantly outside the potential barrier surrounding the impurity. Calculations of the hyperfine splitting and of the A-shell superhyperfine coupling constants as a function of the electric field complete the work.
2006
INFM
QUANTUM COMPUTER
SEMICONDUCTORS
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.14243/115773
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