=. Ero, 663 + 0

{. Eu, *. T. , !. , and !. , 88) û"il,r 'û"i!,r'{-r, r'1,r'fiÏ,r'û"*r, oe,ô)= Jfi .*, Yr-r (r,C) = .lesin d exP

. Jr-'jrr and . Jty, Les matrices ci-dessus peuvent être utilisées également dans des produiB, on obtient alon: -à partir de f. o Ir: f'T-:T=PX+QY'+RZ

Y. Jry, J,l',rj-ljl r{, T-r p= 1f3 u -v)p=[ 3( Iri-Iri ) -( 3 r;]-rrt) lr,' =6I;-fr* g--1f3u+v)(f -6rri-f r

. Joj, +. Jr, A. M. Références-bibliographiques, A. Stegun, and T. Functionsn, En résumé, les 16 matrices de base sont: lf T+

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E. U. Condon and G. H. Et-shortley, The Theory of Atomic Spectra, American Journal of Physics, vol.20, issue.6, 1935.
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G. Is and R. Im, Table of integrals series and produc6, 1965.

K. Rs, Theory of excitons', solid staûe phpics, suppl

E. , F. Seitz, and D. Turnball-), Academic press, 1963.

G. F. Kosrer, (. J. Dimmocr, and W. R. , ?roperties of the Thirty-Two Point Groups, M.LT. press, cambridge, p.lvîassachusetts, 1963.

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P. R. Cernogora, J. , G. J. Benoit, A. La-gi-',-illai-',, M. C. et al., Proc. l7-th lûternar" @nf. Phys. Semicond, p.4, 1959.

R. D. Et and T. C. , ExciOns : Their Pnoperties aûd frses, p.213