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od . So loops with multiple guards are easily rewritten as while statements. But, as in the case of conditional statements, multiple guards improve readability as well as helping to avoid error.

5.16 IMPURITY OCCUPANCY STATISTICS Any book on solid state physics, for example Kasap [124] (page 314) or Sze [44] (page 16), gives the number of free electrons introduced into a crystal due to doping as the integral over the entire conduction band of the density of states multiplied by the probability of occupation:

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where the density of states p(E) (derived earlier in Section 2.3) is written in relation to the conduction band edge Ec as:

Invariants and Bound Functions. When constructing loops, the notions of an invariant property and a bound function1 are crucial. Loops are designed so that

,pp,

and the Fermi-Dirac^ distribution function f ( E ) is approximated by a Boltzmann distribution function:

to be confused with bound variable. The word 'bound' is used in two different ways. In 'bound variable', it signifies 'binding', i.e. tying together. In 'bound function', it signifies a restriction or limitation.

tThis is the true Fermi-Dirac distribution function for a doped semiconductor and not the quasi-function introduced earlier to describe the distribution of electrons within a subband.

(4.14)

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each iteration of the loop body maintains the invariant whilst making progress to the required postcondition by always decreasing the bound function. Let us formulate this design principle in detail. Suppose a problem is specified by precondition P and postcondition Q. We design a loop to meet this specification by identifying an invariant property inv and a bound function bf. The bound function is a measure of the size of the problem to be solved. It is required to be an integer-valued function of the program variables that is guaranteed to be greater than zero when the loop is executed. A guarantee that the value of such a bound function is always decreased at each iteration is a guarantee that the number of times the loop body is executed is at most the initial value of the bound function. The invariant property is designed, in combination with the termination condition, by generalizing the required postcondition. The idea is to split the postcondition, Q, into a termination condition, done say, and the invariant property, inv, in such a way that [inv /\done => Q] . (13.1) (As in the rule for conditional statements, we use square brackets to mean that the property is true in all states.) The termination condition is typically related to the bound function. (Often the termination condition is equivalent to the value of the bound function being zero.) The invariant should also guarantee that, in all states, the value of the bound function is greater than zero, unless the loop has terminated. That is, [inv => bf>0vdone] . (13.2) The invariant property is chosen so that it is easy to design an initialization statement, S, that establishes the invariant property inv. That is, we construct S such that

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The number of free electrons (which is the same as the number of ionised donors) then follows as:

{ P } S { inv } . (13.3)

which leads to (see Kasap [124] (page 314)):

N ii. Find the output unit Ok for which the distance dk,p is the smallest. iii. Update all the weights for the neighborhood Kkp using equation (4.13). (b) Update the learning rate. (c) Reduce the neighborhood radius at specified learning iterations. (d) If stopping conditions are satisfied, stop training; otherwise go to step 2.

The design is completed by constructing a loop body T that maintains the invariant whilst making progress towards the termination condition. That is, using the ghost variable C to relate the values of the bound function before and after execution of T, we construct T to satisfy the specification { inv A -<done A bf = C } T { inv A (bf <C v done) } . (13.4) (Note that (13.4) allows execution of T to not decrease the bound function, provided that done becomes true.) If the termination condition, done, the bound function, bf, the invariant, inv, and the loop body, T, have all been constructed so as to satisfy (13.1), (13.2) and (13.4), it is the case that

where Nc is known as the 'effective density of states' and is given by:

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