2014
DOI: 10.1063/1.4871757
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The effective density of randomly moving electrons and related characteristics of materials with degenerate electron gas

Abstract: Interpretation of the conductivity of metals, of superconductors in the normal state and of semiconductors with highly degenerate electron gas remains a significant issue if consideration is based on the classical statistics. This study is addressed to the characterization of the effective density of randomly moving electrons and to the evaluation of carrier diffusion coefficient, mobility, and other parameters by generalization of the widely published experimental results. The generalized expressions have bee… Show more

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Cited by 15 publications
(15 citation statements)
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“…It illustrates that the effective density of randomly moving electrons eff n equals the total density of free electrons only when the shallow donor density D n is smaller than 18 10 cm −3 . However, a sharp decrease is found at high densities, and the ratio eff n n is well below unity at 21 10 n ≈ cm −3 . The effective density of randomly moving electrons eff n dependence on the total density n of free electrons in nSi at 300 T = K is shown in Figure 5.…”
Section: Applications Of the Basic Relations To Transport Features Ofmentioning
confidence: 92%
See 1 more Smart Citation
“…It illustrates that the effective density of randomly moving electrons eff n equals the total density of free electrons only when the shallow donor density D n is smaller than 18 10 cm −3 . However, a sharp decrease is found at high densities, and the ratio eff n n is well below unity at 21 10 n ≈ cm −3 . The effective density of randomly moving electrons eff n dependence on the total density n of free electrons in nSi at 300 T = K is shown in Figure 5.…”
Section: Applications Of the Basic Relations To Transport Features Ofmentioning
confidence: 92%
“…where both sides mean the conductivity. But as it will be shown later the quantity d d F n E in Equation (2) left side is proportional to the effective density of randomly moving electrons, while the expression enµ contains the total electron density n ; this is wrong for degenerate silicon because the main contribution comes from the randomly moving electrons, located near the Fermi energy, while the contribution due to the electrons located deep below the Fermi level is next to zero because of limitations induced by the Pauli principle [19]- [21]. The randomly moving electrons not only determine the electric conduction and electron diffusion, but also electron heat capacity, electron thermal noise, electron heat conduction and other dissipative phenomena [22].…”
Section: Introductionmentioning
confidence: 99%
“…According to Fermi-Dirac statistics and Pauli principle description of the electrical conductivity of the metals including all valence electrons is unacceptable [9,10], because randomly can move only a small part of electrons which energy is close to the Fermi level energy, and that electrons which energy is well below the Fermi level energy cannot change their energy, because all neighbor energy levels are occupied. Concerning that the Sommerfeld's model is based on the spherical Fermi surface, there also are uncertainties in determination of both the density-of-states (DOS) in conduction band and the Fermi energy, because the Fermi surfaces for many of metals are not spherical [11].…”
Section: Introduction mentioning
confidence: 99%
“…Concerning that the Sommerfeld's model is based on the spherical Fermi surface, there also are uncertainties in determination of both the density-of-states (DOS) in conduction band and the Fermi energy, because the Fermi surfaces for many of metals are not spherical [11]. The determination of the effective density neff of the randomly moving (RM) electrons in elemental metals eliminates the mentioned uncertainties [9,10].…”
Section: Introduction mentioning
confidence: 99%
“…Obviously, this phenomenon is a typical nonlinear effect.Furthermore, the numerical results of energy gap can be used to calculate the number of superconducting carriers. By taking into account the thermal population of the quasiparticle excitations of the Cooper pairs (Bogoliubov quasiparticles), BCS theory predicts:17,18…”
mentioning
confidence: 99%