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Luttinger–Kohn model : ウィキペディア英語版
Luttinger–Kohn model
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.
In this model the influence of all other bands is taken into account by using Löwdin's perturbation method.〔

== Background ==

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 \phi^_:
:\phi = \sum^_ a_ \phi^_
Assuming the unperturbed eigenstates are orthonormalized, the eigenequation are:
:(E-H_)a_m = \sum^_H_a_ + \sum^_H_a_,
where
:H_ = \int \phi^_ H \phi^_d^3 \mathbf = E^_\delta_+H^_.
From this expression we can write:
:a_ = \sum^_ \frac} a_ + \sum^_ \frac} a_ ,
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 a_ for ''m'' in class A, we may eliminate those in class B by an iteration procedure to obtain:
:a_ = \sum^_ \frac - H_} ,
:U^_ = H_ + \sum^_ \frac} \fracH_ })} + \ldots
Equivalently, for a_ ( n \in A ):
:a_ = \sum^_ (U^_ - E\delta_)a_ = 0, m \in A
and
: a_ = \sum^_ \frac - H_\delta_} = 0, \gamma \in B .
When the coefficients a_ belonging to Class A are determined so are a_ .

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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