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149, 647 (1966). G. OvANDER: Soy. -Solid State 4, 112 0962). S. , R. LoUDON: Rev. Mod. Phys. 44, 18 (1972). T. L. FAUST: Appl. Phys. 1,241 (1973). CowLEY:Advan. Phys. 12,421(1963). CoWLEY: Proc. Phys. Soc. 84, 281 (1964). MAR'rIN: Phys. Rev. B4, 3676 (1971). D. Dow, E. 7], p. 33. A. PINcZUK, E. BURSTEIN: Proc. 10th Intern. Conf. , 1970 (US Atomic Energy Commission, 1970), p. 727. L. BmMAN: Phys. Rev. 162, 806 (1967). B. L. BmMAN:Phys. Rev. BI, 1678 (1970). TING, J. B~RMAN: Phys. Rev. BI0, 1725 (1974).

In addition, we have to con- 46 A. P1NCZUK and E. BURSTE1N sider the cases in which the intermediate electronic excitations are either uncorrelated electron-hole pairs, or discrete or continuum exciton states. Let us consider first the case in which the intermediate states are uncorrelated electron-hole pairs. 25] (see [Ref. 1, Sect. 0]). 53) = T-(ie/q)(-~ + I) i (e [exp(iq. 50). The ( - ) and ( + ) signs correspond to the electron and hole contributions, respectively. 50), are the components of the amplitude of the polariton macroscopic electric field.

Rev. 164, 1081 (1967). S. Go, H. Btez, M. CARDONA: Phys. Rev. Letters 34, 580 (1975). R. MARADUDm: Solid State Commun. 8, 859 (1970). CARDOYA: Solid State Commun. 9, 819 (1971). R. LouDON: Proc. Roy. Soc. A275, 218 (1963). R. I~UOON: J. Phys. 26, 677 (1965). B. BENEDEK, K. FRITSCH : Phys. Rev. 149, 647 (1966). G. OvANDER: Soy. -Solid State 4, 112 0962). S. , R. LoUDON: Rev. Mod. Phys. 44, 18 (1972). T. L. FAUST: Appl. Phys. 1,241 (1973). CowLEY:Advan. Phys. 12,421(1963). CoWLEY: Proc. Phys. Soc.

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