The deformation potential theory for the valence bands is different from that
for the conduction bands because of the degeneracy of the valence bands at the
valence band maximum. The operators
are no longer
scalars. Instead, they can be expressed as matrices. Due to symmetry
the six independent operators have only three independent entries, usually
labeled or , depending on the used basis for the
eigenfunctions [Cardona66].
In the basis
with denoting the spin state
( for ) and (
for ), the matrix of the
perturbation Hamiltonian is
|
(3.56) |
with
denoting the matrix
|
(3.57) |
In Section 3.6.1 and Section 3.6.2 it was shown that from
deformation potential theory simple analytical expressions can be derived
for the conduction band shifts induced by an arbitrary strain
tensor
. For the valence band the expressions for the strain-induced
shifts of the heavy-hole, light-hole, and split-off band are more complex,
which limits their practical use [Balslev66].
E. Ungersboeck: Advanced Modelling Aspects of Modern Strained CMOS Technology