Abstract:Abstract. We investigale current fluctuations in non-degenerate Semiconductors, on length scales intermediate between t he elastic and inelastic mean free paths. The shot-noise power P is suppressed below the Poisson value Ppoiasoa -2e7 (afc mean current 7) by the Coulomb repulsion of the carriers. We consider a power-law depenclence of the elastic scattering time τ oc ε α on kinetic energy ε and present an exact solution of the non-linear kinetic equations in the regime of space-charge limited conduction. The… Show more
“…An analytic theory of shot noise in these conductors was proposed by Beenakker [260], and subsequently by Nagaev [261] and Schomerus, Mishchenko, and Beenakker [262,263]. The general conclusion is as follows.…”
Section: E Shot Noise In Non-degenerate Conductorsmentioning
confidence: 91%
“…Furthermore, they do depend on the disorder, and this dependence enters through their sensitivity to the energy dependence of the relaxation time 60 , as noticed by Nagaev [261]. Schomerus, Mishchenko, and Beenakker [263] investigated the case τ (E) ∝ E α , −1/2 ≤ α ≤ 1, which are the only values of α compatible with the regime of space-charge limited conduction. In particular, α = −1/2 corresponds to scattering on short-ranged impurities.…”
Section: E Shot Noise In Non-degenerate Conductorsmentioning
Theoretical and experimental work concerned with dynamic fluctuations has developed into a very active and fascinating subfield of mesoscopic physics. We present a review of this development focusing on shot noise in small electric conductors. Shot noise is a consequence of the quantization of charge. It can be used to obtain information on a system which is not available through conductance measurements. In particular, shot noise experiments can determine the charge and statistics of the quasiparticles relevant for transport, and reveal information on the potential profile and internal energy scales of mesoscopic systems. Shot noise is generally more sensitive to the effects of electron-electron interactions than the average conductance. We present a discussion based on the conceptually transparent scattering approach and on the classical Langevin and BoltzmannLangevin methods; in addition a discussion of results which cannot be obtained by these methods is provided. We conclude the review by pointing out a number of unsolved problems and an outlook on the likely future development of the field.
“…An analytic theory of shot noise in these conductors was proposed by Beenakker [260], and subsequently by Nagaev [261] and Schomerus, Mishchenko, and Beenakker [262,263]. The general conclusion is as follows.…”
Section: E Shot Noise In Non-degenerate Conductorsmentioning
confidence: 91%
“…Furthermore, they do depend on the disorder, and this dependence enters through their sensitivity to the energy dependence of the relaxation time 60 , as noticed by Nagaev [261]. Schomerus, Mishchenko, and Beenakker [263] investigated the case τ (E) ∝ E α , −1/2 ≤ α ≤ 1, which are the only values of α compatible with the regime of space-charge limited conduction. In particular, α = −1/2 corresponds to scattering on short-ranged impurities.…”
Section: E Shot Noise In Non-degenerate Conductorsmentioning
Theoretical and experimental work concerned with dynamic fluctuations has developed into a very active and fascinating subfield of mesoscopic physics. We present a review of this development focusing on shot noise in small electric conductors. Shot noise is a consequence of the quantization of charge. It can be used to obtain information on a system which is not available through conductance measurements. In particular, shot noise experiments can determine the charge and statistics of the quasiparticles relevant for transport, and reveal information on the potential profile and internal energy scales of mesoscopic systems. Shot noise is generally more sensitive to the effects of electron-electron interactions than the average conductance. We present a discussion based on the conceptually transparent scattering approach and on the classical Langevin and BoltzmannLangevin methods; in addition a discussion of results which cannot be obtained by these methods is provided. We conclude the review by pointing out a number of unsolved problems and an outlook on the likely future development of the field.
“…This would change the energy dependence of the diffusion constant from D ∝ ε to D ∝ ε 2−d/2 . The shot-noise power remains unaffected for d = 2, but for d = 3 one obtains [12] P/P Poisson = 0.407 -some 20% above the value for an ε-independent scattering rate. Concerning the experimental observability, the main obstacle is the tendency of electron-phonon scattering to equilibrate the electron gas at the lattice temperature.…”
A theory is presented for the universal reduction of shot noise by Coulomb repulsion, which was observed in computer simulations of a disordered non-degenerate electron gas by González et al. [Phys. Rev. Lett. 80, 2901]. The universality of the reduction below the uncorrelated value is explained as a feature of the high-voltage regime of space-charge limited conduction. The reduction factor depends on the dimensionality d of the density of states, being close but not quite equal to 1/d in two and three dimensions.
“…In the latter case (γ in,φ negative), the values of γ depend on the competition between the diagonal and the off-diagonal contributions. For nondegenerate systems (for which γ in = 1), the presence of diagonal and off-diagonal terms explains the actual scenario taken by the Fano factor, which, according to the dimensionality in momentum space and the energy dependence of the relaxation time, was found to run from suppressed to enhanced values [15,16,18,19,22]. In contrast, for degenerate systems these effects have not been investigated to our knowledge.…”
Section: Discussionmentioning
confidence: 95%
“…The presence of electron-electron scattering was found to provide a √ 3/4 suppression factor [13,14]. Also, nondegenerate mesoscopic conductors were found to exhibit shot-noise suppression due to the presence of long-range Coulomb interactions, and a suppression factor of 1 3 , or very near to this value, was predicted by Monte Carlo calculations [15] and interpreted analytically [16][17][18]. In particular, the dimensionality in momentum space [15][16][17]19] and an energy-dependent scattering time [16,17,[19][20][21][22] were found to give different suppression values, thus washing out the universality features of suppression.…”
The role played by boundary conditions at a kinetic level in determining the noise properties of mesoscopic diffusive conductors is evaluated by decomposing the current fluctuations, into fluctuations of boundaries, self-consistent electric potential and the intrinsic Langevin source. We show that the self-consistent contribution is essentially controlled by the range of energies determined by the distribution function at the contacts together with the differential conductivity in energy space. The intrinsic contribution is completely determined by the boundary conditions and is expressed in closed analytical form in these terms. The present formulation provides a unifying microscopic approach of the noise properties of mesoscopic diffusive conductors showing that (i) in the absence of Coulomb interaction the Fano factor γ takes values bounded in the range 1 3 γ 1 and (ii) in the presence of Coulomb interaction the values of γ are no longer bounded in the above range and enhanced shot noise becomes possible.
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