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Titlebook: Spin-orbit Coupling Effects in Two-Dimensional Electron and Hole Systems; Roland Winkler Book 2003 Springer-Verlag Berlin Heidelberg 2003

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Roland Winklerisotopes can be easily understood from the single particle Nilsson diagram (see e.g. refs [3,4]). The large (about 1.5 MeV) Z=34 gaps appear both at prolate and oblate shapes, at N = 38 the gap opens at large prolate shapes while oblate configurations in Se are stabilized by the N = 36 shell gap.
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Roland Winklerisotopes can be easily understood from the single particle Nilsson diagram (see e.g. refs [3,4]). The large (about 1.5 MeV) Z=34 gaps appear both at prolate and oblate shapes, at N = 38 the gap opens at large prolate shapes while oblate configurations in Se are stabilized by the N = 36 shell gap.
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Roland Winklerisotopes can be easily understood from the single particle Nilsson diagram (see e.g. refs [3,4]). The large (about 1.5 MeV) Z=34 gaps appear both at prolate and oblate shapes, at N = 38 the gap opens at large prolate shapes while oblate configurations in Se are stabilized by the N = 36 shell gap.
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Electron and Hole States in Quasi-Two-Dimensional Systems,In Chapters 2 and 3 we introduced the general concepts for characterizing the semiconductor band structure and a model for calculating it. In the present chapter we shall discuss the applications of this model to quasi-2D semiconductor quantum structures.
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Notation and Symbols,Appendix: Notation and Symbols
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