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2
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note
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If one takes into account the Zeeman splitting of each LL, the partial filling factors of the lower and upper spin branches of the n-th LL are, respectively, v̄ = v - 2n and v̄ = v - (2n + 1).
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Inter-LL excitations may be included in the random-phase approximation. This leads to a screened Coulomb interaction in a certain wave vector range but has only a minor influence on the physical properties of the system; see: ALEINER I. L. and GLAZMAN L. I., Phys. Rev. B, 52 (1995) 11296.
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