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The conduction and valence bands of CuCl are parabolic and nondegenerate, with both extrema at κ = 0, opposite parities, and hole effective mass heavier than the electron one; as a consequence, exciton and biexciton in CuCl are a solid-state analogue of atomic and molecular hydrogen. J. B. Grun et al., in Excitons, edited by E. I. Rashba and M. D. Sturge (North-Holland, Amsterdam, 1982), Chap. 11; J. K. Pribram, G. L. Koos, F. Bassani, and J. P. Wolfe, Phys. Rev. B 28, 1048 (1983); M. Ueta et al., Excitonic Processes in Solids, Springer Series in Solid-State Sciences Vol. 60 (Springer-Verlag, Berlin, 1986).
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The conduction and valence bands of CuCl are parabolic and nondegenerate, with both extrema at κ = 0, opposite parities, and hole effective mass heavier than the electron one; as a consequence, exciton and biexciton in CuCl are a solid-state analogue of atomic and molecular hydrogen. J. B. Grun et al., in Excitons, edited by E. I. Rashba and M. D. Sturge (North-Holland, Amsterdam, 1982), Chap. 11; J. K. Pribram, G. L. Koos, F. Bassani, and J. P. Wolfe, Phys. Rev. B 28, 1048 (1983); M. Ueta et al., Excitonic Processes in Solids, Springer Series in Solid-State Sciences Vol. 60 (Springer-Verlag, Berlin, 1986).
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The conduction and valence bands of CuCl are parabolic and nondegenerate, with both extrema at κ = 0, opposite parities, and hole effective mass heavier than the electron one; as a consequence, exciton and biexciton in CuCl are a solid-state analogue of atomic and molecular hydrogen. J. B. Grun et al., in Excitons, edited by E. I. Rashba and M. D. Sturge (North-Holland, Amsterdam, 1982), Chap. 11; J. K. Pribram, G. L. Koos, F. Bassani, and J. P. Wolfe, Phys. Rev. B 28, 1048 (1983); M. Ueta et al., Excitonic Processes in Solids, Springer Series in Solid-State Sciences Vol. 60 (Springer-Verlag, Berlin, 1986).
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Biexciton states having a larger wave vector, and a faster dephasing, could be accessed in a copropagating pump and probe configuration.
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