Electron theory of the optical properties of laser-excited semiconductors

[1]  J. Callaway Quantum theory of the solid state , 1974 .

[2]  H. Haug,et al.  Two-Photon Generation of Excitonic Molecules and Optical Bistability , 1981 .

[3]  Stefan Schmitt-Rink,et al.  Ionization of the Direct-Gap Exciton in Photoexcited Germanium , 1983 .

[4]  N. Peyghambarian,et al.  Biexciton resonance linewidth in CuCl: Collision broadening or not? , 1982 .

[5]  W. Schäfer,et al.  Transient Optical Spectra of a Dense Exciton Gas in a Direct-Gap Semiconductor , 1982 .

[6]  M. Rösler,et al.  Theory of Electron–Hole Plasma in CdS , 1976 .

[7]  R. Der,et al.  The influence of two‐particle states (excitons) on the dielectric function of the electron—hole plasma , 1979 .

[8]  V. Asnin,et al.  Direct absorption inside the electron‐hole liquid in Ge: Warping effects and final state interactions , 1981 .

[9]  B. Seraphin Optical Properties of Solids: New Developments , 1976 .

[10]  David A. B. Miller,et al.  Optical bistability and signal amplification in a semiconductor crystal: applications of new low‐power nonlinear effects in InSb , 1979 .

[11]  Hyatt M. Gibbs,et al.  Optical bistability in semiconductors , 1979 .

[12]  R. Zimmermann,et al.  Dynamical screening and self‐energy of excitons in the electron–hole plasma , 1978 .

[13]  Stuart A. Rice,et al.  Quantum Statistical Mechanics , 1963 .

[14]  G. Mahan Many-particle physics , 1981 .

[15]  R. Zimmermann,et al.  Influence of Exciton Gas and Electron—Hole Plasma on Exciton Energy Levels , 1980 .

[16]  D. Pines,et al.  The theory of quantum liquids , 1968 .

[17]  Nevill Mott,et al.  Metal-insulator transitions , 1974 .

[18]  Nasser N Peyghambarian,et al.  Observation of Biexcitonic Optical Bistability and Optical Limiting in CuCl , 1983 .

[19]  W. Ekardt,et al.  Many‐exciton effects in the theory of biexcitons , 1978 .

[20]  A. Mysyrowicz,et al.  Direct creation of high-density biexcitons at K = 0 in CuCl (A) , 1979 .

[21]  Lev P. Gor'kov,et al.  Quantum field theoretical methods in statistical physics , 1967 .

[22]  K. Shindō Effective Electron-Hole Interaction in Shallow Excitons , 1970 .

[23]  W. Ekardt,et al.  Theory of Biexcitons Using the Boson Formalism The Ground State Binding Energy , 1976 .

[24]  H. Haug,et al.  Many-Body Theory of Optical Bistability in Semiconductors , 1982 .

[25]  G. A. Thomas,et al.  The Electron-Hole Liquid in Semiconductors: Experimental Aspects , 1978 .

[26]  M. Combescot,et al.  The dielectric constant and plasma frequency of p-type Ge like semiconductors , 1972 .

[27]  H. Sumi,et al.  Urbach-Martienseen Rule and Exciton Trapped Momentarily by Lattice Vibrations , 1971 .

[28]  H. Haug,et al.  Nonlinear Energy Transport of Radiation in Dielectrics Due to Virtual Biexciton Formation , 1981 .

[29]  C. Blomberg,et al.  Single Particle Green's Function in the Electron–Plasmon Approximation , 1973 .

[30]  E. Hanamura Optical bistable system responding in pico-second , 1981 .

[31]  A. Mysyrowicz,et al.  Evidence for Bose-Einstein Statistics in an Exciton Gas , 1980 .

[32]  R. Zimmermann,et al.  Correlated Hartree-Fock Theory of the Electron—Hole Plasma Containing Exciton Bound States , 1981 .

[33]  M. P. Tosi,et al.  Correlations in Electron Liquids , 1982 .

[34]  R. Zimmermann,et al.  Correlated pairs and a mass action law in two‐component Fermi systems excitons in an electron‐hole plasma , 1979 .

[35]  R. Zimmermann Excitons and Electron‐Hole Plasma. A Ground State Calculation , 1976 .

[36]  J. Bigot,et al.  Optical bistability due to biexcitons in CuCl , 1983 .

[37]  V. May,et al.  Renormalization of polaritons due to virtual formation of biexcitons at high densities of excitation , 1979 .