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is to change from the |X T), |Y T), |Z |), |X j), |Y j}, |Z |) basis into another one, such that its member functions are simultaneously the eigenstates of the angular momentum operator (with eigenvalues J equal to 3h/2 or h/2), and of its projection along the z-axis mj (with eigenvalues equal to 3/2 or 1/2). This is achieved by making appropriate linear combinations of the atomic basis states. The list of this new set of | J, mj) basis states is given below in equation (10.1). The precise form of the Hamiltonian depends on the pre-factors in equation (10.1), for example the presence of the imaginary number i or 1 does not change the state properties, and it also depends on how these states are ordered in the list. There is no unique choice that is universally accepted in the literature, however one of the frequently used possibilities, see for example [228], which will be adopted here, reads:

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= M-=-2 } .

If two objects are indiscernible over a set of attributes, it means that the objects have the same values for these attributes Formally, the indiscernibility relation is defined as: IND(B) = {(z,y) 6 U2\a(x) = a(y) Va B} where B C A With U/IND(B) is denoted the set of equivalence classes in the relation IND(B) That is, U/IND(B) contains one class for each set of objects that satisfy IND(B) over all attributes in B Objects are therefore grouped together, where the objects in different groups cannot be discerned between A discernibility matrix is a two-dimensional matrix where the equivalence classes form the indices, and each element is the set of attributes which can be used to discern between the corresponding classes.

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Just as with the original (|X T), |Y T), |Z T), |X j}, |Y j}, |Z | states, the new basis states are all orthogonal to each other. In this | J, mj) basis the 6 x 6 Hamiltonian that describes the HH, LH and SO bands for the bulk reads:

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Note that the middle assertion could now be omitted. It is included in order to document the program better. Exercise 10.21. This exercise is a variation on Exercise 10.12. Recall the statement of the problem. A program has two real variables x and y and one integer variable k. Initially, k is strictly positive. It is required to decrease the value of k to a positive value whilst maintaining the value of xk x y constant. In this exercise, the requirement is to develop a program that is the sequential composition of two statements using the fact that decreasing an odd number by one always yields an even number. Construct statement 52 and assertion P such that executing S2 beginning in a state satisfying P A even.fe A xkxy = C is guaranteed to terminate in a state satisfying 0 ^ f c < K A xkxy = C . (10.23) (10.22)

where k = kx iky, 71,2,3 are the Luttinger parameters, and ASO is the spin orbit splitting the spacing between the HH (or LH) band and the SO band at the (k = 0)

(Hint: a simple assignment statement is all that is needed make use of Exercise 10.11. You can then use the assignment axiom to determine what P should be.) Now construct statement SI with precondition 0 < k = K A xkxy = C (10.24)

Formally, for a set of attributes B C A in A = (U, A), the discernibility matrix M D ( B ) is defined as MD(B) = {mD(i,j)}nxn for 1 < i,j < n, and n = \U/IND(B}\, with rnD(i, j) = {a e B\a(Ei) ^ a(Ej}} for i, j = 1, , n; a(Ei) indicates that attribute a belongs to equivalence class Ei Using the discernibility matrix, discernibility functions can be defined to compute the minimal number of attributes necessary to discern equivalence classes from one another The discernibility function f(B), with B C A, is defined as.

F-point. The values of 71,2,3 and ASO in some common semiconductors are given in Table 10.1. In writing equation (10.2) the convention has been used that the hole energy is measured from the top of the valence band downwards (the inverted energy picture). This is because it is usually easier to look at the hole band structure in the same manner as that for electrons, and this is possible if only holes are considered. For the true energy picture (as in Fig. 10.1), all the terms in the Hamiltonian should be multiplied by -1. Furthermore, it is important to note that the coordinate system in which this Hamiltonian is written is not oriented arbitrarily the axes x, y, and z are aligned along the edges of the crystalline cubic unit cell. The Schrodinger equation corresponding to this Hamiltonian may still be written as

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