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This quantity includes lecture notes and chosen contributed papers awarded on the overseas summer time institution on New advancements in Semiconductor Physics held on the collage of Szeged, July 1-6, 1979. the key a part of the contributions during this quantity is said to the recent experimental technics and theoretical rules utilized in learn of recent semiconductor fabrics, in most cases III-V semiconductors.
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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.
Bogoliubov New Method in the theory of SC