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The split-off states not only are farther in energy but their mass is not as light as that of LHs which, as we explain below, is central to originate the characteristic behavior of holes in CQDs.
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The split-off states not only are farther in energy but their mass is not as light as that of LHs which, as we explain below, is central to originate the characteristic behavior of holes in CQDs.
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In the absence of external magnetic fields, | Fz, ν= k and | - Fz, ν= ,k are degenerate (Kramer doublets) (Ref.). For example, the ground state | 3/2, 1 is degenerate with | -3/2, ,1 . For simplicity of the discussion, in the main text we only discuss the Fz =3/2 states. The reasoning for Fz =-3/2 would be analogous.
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In the absence of external magnetic fields, | Fz, ν= k and | - Fz, ν=,k are degenerate (Kramer doublets) (Ref.). For example, the ground state | 3/2, 1 is degenerate with | -3/2, 1. For simplicity of the discussion, in the main text we only discuss the Fz =3/2 states. The reasoning for Fz =-3/2 would be analogous.
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For the Fz =-3/2 Kramer-degenerate states the relationship is reversed: ν= corresponds to "almost antisymmetric" and ν= to "almost symmetric."
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For the Fz =-3/2 Kramer-degenerate states the relationship is reversed: ν= corresponds to "almost antisymmetric" and ν= to "almost symmetric."
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