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Where m* is the band-edge effective mass, k is Boltzmann constant, T is the lattice absolute temperature, h is Plank constant divided by 2, Tu* Tu gives the tunneling probability density of the outgoing electron, F is Fermi energy level, l is energy of the electron associated with longitudinal wave vector of the electron in the conduction band, V is the applied voltage.
In this paper we find out the basic solid state parameters like penn gap, plasma energy, polarizability and fermi energy for calcium boro lactate crystals.
The Plasma energy in relation to Penn gap and Fermi energy [7] is termed as
37)], is representative of the Fermi energy of metals, namely it is close to the Fermi energy of the copper crystal.
We think that we may associate to the Fermi energy [E.
As we can see from equation (20), this quasi-particle has a mass-energy equal to the Fermi energy divided by the number of cells in the string.
However, because the conduction [GAMMA] sub-band band in GaSb is not the dominant band for determining the Fermi energy, its non-parabolicity correction may not have a significant effect on the results given below and may lie within the uncertainties associated with the band masses quoted in the literature for GaSb.
Tables 1 and 2 contain the input parameters for the calculations of the Fermi energy as a function of the dopant donor density.
A figure that compares the calculated total electron density as a function of the Fermi energy with the fitting results from Eq.
In graphene, the energy bands touch the Fermi energy at six discrete points at the edges of the hexagonal Brillouin zone.
F] is the Fermi energy, m* is the effective mass of electrons with energy E, and [?