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G is one of the roots of the equation in x x2-x-l = 0 . (In other words, G 2 -G-1 = 0.) The other root is G' = i ( l - A / 5 ) . Here we use strong induction to prove that, for all n such that n ^ 1, Gn~2 ^ F.n ^ Gn~l . The exercises ask you to prove further properties of F.n. Basis. It is important to be very careful in the proof of any theorem about the Fibonacci numbers because there are three separate cases in the definition; it is very easy to make the mistake of applying the rule F.(n+2) = F.(n+l) + F.n when n is not defined. (See Exercise 12.14 for an example). In addition, in this case, the property we have to prove is claimed to be true only for n such that n^l. (It is false when n equals 0.) A mistake that is easily made in the induction step is to assume that the property is true when n equals 0. This means that we are obliged to prove the property for the cases n - 1 and n = 2 before proceeding to the induction step. For n = 1, we have

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components learning is an extension of the Hebbian learning rule, referred to as normalized Hebbian learning, to include a feedback term to constrain weights. In doing so, principal components could be extracted from the data. The weight change is given as

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where NQU and NoB are constants (220 and 880 meV respectively in Cd1_xMnxTe). The expectation value of the magnetic ion spin along the z-axis (Sz) is given by: where So (x) is the effective spin of the magnetic ions and B j is a Brillouin function describing the response of the spins in a magnetic fields B. The effective spin So accounts for the proportion of magnetic ions which are spin-paired with a nearest neighbour and can not respond to the alignment induced by the magnetic field. Alternatively the effective spin can be considered as the concentration of spin-singlet states, i.e. where the spin of the Mn2+ ions are 5/2. Recent theoretical studies [117] have calculated x in agreement with experiment [118] and shown that for moderate fields (=8 T), i.e. when the splittings have saturated, but before the nearest neighbour spin pairings are broken, the maximum value of x (Sz(x)} occurs at a manganese concentration x = 0.15 and is equal to 0.105. Hence, in Cd1_xMnxTe the maximum splitting in the conduction band is = 23 meV, and for the heavy-holes in the valence band it is =92 meV. The paramagnetic behaviour falls off with increasing temperature. When applying a magnetic field to a semiconductor heterostructure, the direction of the field becomes important. For fields parallel to the growth axis (z-) (the Faraday configuration), the splittings are still well represented by Fig. 5.20. However, application of the magnetic field along the plane of the wells, i.e. the Voigt configuration, leads to mixing of the light- and heavy-hole valence states, thus producing a

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G 1 - 2 < F.I < G1"1

much more complex band structure. However, this lies beyond the scope of this short introduction. Thus far, the CdTe/Cd1_xMnxTe system has been employed to illustrate donor binding energy calculations; now, however, specific use will be made of these magnetic properties in an application of the binding-energy calculations, namely spin-flip Raman spectroscopy. 5.11.2 Spin-flip Raman spectroscopy

arithmetic, definition of F.I } G = ^(l + A/5) > l.SoG- 1 < 1. }

= uki(t)

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