By Domingo A. Herrero

The aim of this monograph (and a moment one, by way of C. Apostol,

L. A. Fialkow, D. A. Herrero and D. Voiculescu that would persist with and

complete the consequences contained the following) is to supply a suite of normal

arguments to accommodate approximation difficulties (in the norm-topology)

related to these subsets of the algebra L[H) of all operators performing

on a fancy separable limitless dimensional Hubert area which are

invariant below similarities.

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**Example text**

51). Note that è(-kz) = ë(kz), h(—kz) • q{ = -h(kz) • qu and h(-kz) -pi = -h(kz) •pi. A factor of 2 is obtained. 53/) =Mhh(k±,k'±) k2k'z sin{fa - 4>'k) sin(<^. 535) k' (2) _ First we calculate the second order coherent wave (E s (r)). 54) the second-order coherent wave is in the specular direction. 57) then the cross-polarized component is equal to zero so that there is no depolarization in the coherent reflected wave. To see that, we can set 4>i — 0. Then W depends on cos

In SPM, f ( r ± ) and its derivatives are regarded as small parameters. Thus not only the rms heights are small but also the slopes have to be small. 7) to obtain the set of equations for the different-order solutions. 16) ^ r'±)\ =( » : ^ +s a - I ^ « ) •si-Vj The assumptions are fc/ft), Wft), ^ « 1 (1-2-18) Note that the z components of the surface fields are of a lower order than the horizontal components because of the small slope approximation. 11) and equating the same-order terms, we can calculate the surface fields to the zerothorder, the first-order, and so on.

71). 75a) -oo where a, ß = v, h. 756) f(fc? 75c) 1 + cos{(j)k - 4>'k) cos($. - i) k'\z + Ki /c | k i = • kh lz {k\z + kz)'^ (k\kiz + -sm(4>k-4>'k)sm(4>'k-4>i) fl(k±,ki±) sin(0A. 75 d) s i n ^ - ^ - ^ 2 "'1Z + + cos(<^ - sin(^. - + fc'^)) Also fc kirk? ^ T o ? ( c o s f o f c + (fc;2 + k'zk'u)sm(