A flavor of the k·p perturbation theory used for calculating the structure of multiple, degenerate electronic bands in bulk and quantum well semiconductors. The method is a generalization of the single band k.p theory.
All bands can be subdivided into two classes (Figure 1):
- Class A: six valence bands (heavy hole, light hole, split off band and their spin counterparts) and two conduction bands.
- Class B: all other bands.
The method concentrates on the bands in Class A, and takes into account Class B bands perturbatively.
We can write the perturbed solution as a linear combination of the unperturbed eigenstates :
Assuming the unperturbed eigenstates are orthonormalized, the eigenequation are:
From this expression we can write:
where the first sum on the right-hand side is over the states in class A only, while the second sum is over the states on class B. Since we are interested in the coefficients for m in class A, we may eliminate those in class B by an iteration procedure to obtain:
Equivalentrly, for ():
When the coefficients belonging to Class A are determined so are .
Schrödinger equation and basis functions
The Hamiltonian including the spin-orbit interaction can be written as:
and the perturbation Hamiltonian can be defined as
The unperturbed Hamiltonian refers to the band-edge spin-orbit system (for k=0). At the band edge, conduction band Bloch waves exhibit s-like symmetry, whole valence band states are p-like (3-fold degenerate without spin). Let us denote these states as , and , and respectively. These Bloch functions can be pictured as periodic repetition of atomic orbitals, repeated at intervals correcsponding to the lattice spacing. The Bloch function can be expanded in the following manner
where j' is in Class A and is in Class B. The basis functions can be chosen to be
Using Löwdin's method, only the following eigenvalue problem needs to be solved
The second term of can be neglected compared to the similar term with p instead of k. Similarly to the single band case, we can write for
We now define the following parameters
and the band structure parameters (or the Luttinger parameters) can be defined to be
These parameters are very closely related to the effective masses of the holes in various valence bands. and describe the coupling of the , and states to the other states. The third parameter relates to the anisotropy of the energy band structure around the point when .
Explicit Hamiltonian matrix
The Luttinger-Kohn Hamiltonian can be written explicitly as a 8X8 matrix (taking into account 8 bands - 2 conduction, 2 heavy-holes, 2 light-holes and 2 split-off)
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