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Note that the step from Eq. (20.52) to (20.53) involves approximations that are not detailed further here. It leads to a result that is somewhat similar to the result of [Ayadi et al. 2002]
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1. We first count states in k space; this is the fundamentally correct way to count quantum states. 2. Next, we can use the bandstructure E(k) to count states in E space. The rationale for doing so is that the FD probabilities depend on electron energies E, rather than directly on k. For example, we know that near band extrema, we have a parabolic E(k) relationship, which leads to a parabolic density of states in three dimensions. 3. We next multiply the density of states by the Fermi-Dirac distribution function. For electrons in band n in the repeated zone band scheme, where n is the index for K (e.g., valence band, conduction band,) due to quantization inside the primitive cell, we get
the LOLIA, with 7 local base stations, and of FCA using a 7-cell reuse cluster, under a uniform geographic traffic distribution, with and without power control,for 2 and 4 element antenna arrays with beamforming in a multipath environment.
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Hence, in order to minimize I ( f ) over F, suffices to minimize it
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