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15: Remainder Computation struction of the elementary algorithm in Section 15.2 (for both the cases that 0 ^ P and P ^ 0) establishes that there is at least one remainder r and quotient d for all integers P and all strictly positive natural numbers Q. Together, we have thus established that there is a function that maps given integers P and Q, where 0 < Q, to the remainder, r, and quotient, d, after dividing P by Q, as specified formally by (15.1). A specification (a relation between input and output values) has a functional solution if there is exactly one output for each input. Exhibiting an algorithm, no matter how efficient or inefficient, satisfying the specification is the most effective way of demonstrating the existence of at least one solution to a specification. Recognizing that a specification has a functional solution has important consequences for reasoning about the specification. The consequences are realized by naming the function and expressing the functionality by a simple equivalence. (Some logic texts refer to this process as Skolemization.) In the case of the specification (15.1), there are two quantities involved, so we give separate names to each. The standard name in mathematics for the remainder function is 'mod'; the symbol '-r' is used for the quotient. Given integers P and Q, where 0 < Q, P mod Q denotes the remainder, and P + Q denotes the quotient, after dividing P by Q. The existence and uniqueness of these functions is expressed by the calculational rule: r = PmodQ A d = P - Q = 0 ^ r < Q A P = Qxd + r . (15.6)

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If this lattice constant is not equal to that of any readily available substrate then it can be achieved by growth of a suitable buffer layer. For example in the Si1_xGez/Si material system strain-balancing is achieved by growing a buffer layer with the appropriate Ge composition, i.e. Sii_ y Ge y . This is usually linearly graded from the pure silicon composition of the substrate to the required composition y. If a multilayer structure has periodicity, the above expression should be understood in terms of the single period i.e. it should be applied to the n layers constituting a single period, and the whole structure will then clearly be strain balanced. The previous derivation takes into account the difference in elastic properties of the layers (i.e. elastic stiffness constants). If the elastic constants are similar for all layers of the structure then the stain-balancing condition can be simplified by taking into account only the difference of the lattice constants (also known as the 'average lattice method') as:

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Splitting the equivalence into a mutual implication, the '=>' expresses the existence of a solution to (15.1), and the '<=' expresses the uniqueness of a solution to (15.1). We established the existence of a solution by constructing the elementary algorithm of Section 15.2. The uniqueness of the solution was established in Section 15.1. In 6, the symbol' V was used for integer division, but a different definition was given. We show in Section 15.3.3 that the two definitions are equivalent. For the moment, however, we take care to use only properties of -r that are derived from (15.6). The standard convention in mathematics texts is that mod, like -5-, has higher precedence than addition but lower precedence than multiplication. So, for example, m + nmodQ and m + (nmodQ) are equal. Also, raxnmodQ and (raxn) mod Q are equal. Giving multiplication precedence over mod is undoubtedly due to the fact that it is common to denote multiplication by juxtaposition, and the eye naturally groups ra and n together in mnmodQ. When multiplication is explicitly denoted, the algebraic properties make it undesirable to give multiplication precedence over mod. Our own preference is therefore for the opposite convention. However, to avoid confusion with other texts, we take the middle road of including parentheses, even though some may be omitted.

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If the substrate is fixed and cannot be engineered, the quantum well structure itself has to be 'tailored' to match the substrate, the complexity of which depends on the number of different layers per period and the boundaries imposed by the desired application. In something like a quantum well infrared photodetector (QWIP) this could be achieved by altering the width of the thick barrier layer separating the quantum well absorbing regions, as provided the thickness of this layer is above some minimum (to limit the dark current) it's precise value is not too important. In a quantum cascade laser the injector region offers some flexibility to allow a design to be created which also satisfies the strain-balancing condition. 7.4 EFFECT ON THE BAND PROFILE OF QUANTUM WELLS The strain in epitaxial layers acts to change the crystal lattice geometry, i.e. to perturb its size and symmetry. This results in a change of the electronic structure in particular a modification of the conduction and valence band edges and therefore a corresponding shift in the energy levels. In order to give a quantitative measure of this further effect of strain, a general case of the strained crystal is considered under the framework of deformation potential theory. This section will consider the simple case of the conduction band F minimum, while more detailed analysis exploring the valence band will be presented in 10. If the strain is assumed to be small, which is the case in semiconductor quantum wells (~1%), first order perturbation theory can be used to calculate the band shift. The Hamiltonian under strain can be expressed as the sum of the unperturbed Hamiltonian (Ho) and the strain induced contribution (He),i.e.

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