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8.1 FURTHER CONFINEMENT It has already been shown that the reduction in dimensionality produced by confining electrons (or holes) to a thin semiconductor layer leads to a dramatic change in their behaviour. This principle can be developed by further reducing the dimensionality of the electron's environment from a two-dimensional quantum well to a one-dimensional quantum wire and eventually to a zero-dimensional quantum dot. In this context, of course, the dimensionality refers to the number of degrees of freedom in the electron momentum; in fact, within a quantum wire, the electron is confined across two directions, rather than just the one in a quantum well, and, so, therefore, reducing the degrees of freedom to one. In a quantum dot, the electron is confined in all three-dimensions, thus reducing the degrees of freedom to zero. If the number of degrees of freedom are labelled as "Df and the number of directions of confinement are labelled as Dc, then clearly:

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We next consider whether remainder computation distributes through addition. That is, we seek an operator e such that (m+n)modQ = (m mod Q) e (n modQ) . We have = (ra+n)modQ { (15.7) in order to introduce m mod Q }

for all solid state systems. These values are highlighted for the four possibilities shown in Table 8.1. Tradition has determined that the reduced-dimensionality systems are labelled by the remaining degrees of freedom in the electron motion, i.e. T>f, rather than the number of directions with confinement T>c.

Figure 7.4: Huber objective function where ts and tu are respectively the scaled and original unsealed target values, the NN must be trained longer until MSES = (Cl)2MSEr to reach a desired accuracy, [Engelbrecht et al. 1995a]. MSE r ' (7.12)

{ That is,

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Table 8.1 The number of degrees of freedom X>f in the electron motion, together with the extent of the confinement T>c, for the four basic dimensionality systems

(15.12) }

Fig. 8.1 gives a simple outline of how quantum wires might be fabricated, although note that there is more than one method and the interested reader should refer to a specialist growth treatise for further details. A standard quantum well layer can be patterned with photolithography or perhaps electron-beam lithography, and etched to leave a free standing strip of quantum well material; the latter may or may not be filled in with an overgrowth of the barrier material (in this case, Gai-^ AlxAs ). Any charge carriers are still confined along the heterostructure growth (z-) axis, as they were in the quantum well, but in addition (provided the strip is narrow enough) they are now confined along an additional direction, either the x- or the y-axis, depending on the lithography.

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The hyperbolic tangent will therefore result in faster training times than the sigmoid function, assuming the same initial conditions and training data. The scaling process above is usually referred to as amplitude scaling, or min-max scaling. Min-max scaling preserves the relationships among the original data. Two other frequently used scaling methods are mean centering and variance scaling. To explain these two scaling methods, assume that R / x p is a matrix containing all input vectors such that input vectors are arranged as columns in Z, and T E HKxp is the matrix of associated target vectors, arranged in column format. For the mean centering process, compute p

{ (15.26) }

Fig. 8.2 shows an expanded view of a single quantum wire, where clearly the electron (or hole) is free to move in only one direction, in this case along the 7/-axis. Within the effective-mass approximation the motion along the axis of the wire can still be described by a parabolic dispersion, i.e.

(15.26)

Figure 8.2 A single wire and an expanded view showing schematically the single degree of freedom in the electron momentum

the patterns, and T^ is the average target value for the fc-th output unit over all patterns. Then,

addition is symmetric } (15.26) with m,n := n.ramodQ }

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