Electron-phonon scattering time in crystalline disordered Ti1−xAlx alloys

1996 ◽  
Vol 219-220 ◽  
pp. 68-70 ◽  
Author(s):  
J.J. Lin ◽  
C.Y. Wu
2000 ◽  
Vol 26 (12) ◽  
pp. 890-893 ◽  
Author(s):  
V. V. Andrievskiı̆ ◽  
I. B. Berkutov ◽  
Yu. F. Komnik ◽  
O. A. Mironov ◽  
T. E. Whall

1998 ◽  
Vol 09 (01) ◽  
pp. 125-144
Author(s):  
JEAN-PIERRE LEBURTON

The interplay between geometrical confinement and materials considerations can efficiently reduce phonon-assisted transport, enabling scattering time and dissipation engineering in quantum devices. In resonant tunneling (RT) structures, quenching of phonon-assisted transmission leading to considerable reduction of the off-resonance valley-current is shown to occur in interband devices. In structures of low dimensionality such as quantum wires, electron-phonon scattering exhibits size effects and intersubband resonances which modulates the drift velocity and conductance of one-dimensional systems. Quantum dot nanostructures offer large flexibility for reduction and modulation of dissipative processes such as oscillatory hopping conductance induced by acoustic phonons in linear chains of quantum dots or negative differential resistance curve shaping in RT through quantum dot arrays.


2015 ◽  
Vol 14 (02) ◽  
pp. 1550018 ◽  
Author(s):  
Ferdinand Grüneis

We regard a metallic resistor for temperatures T ≫ Θ D (= Debye temperature); under this condition, electron–phonon scattering is the dominant scattering mechanism. We investigate the noise properties under the supposition that phonon scattering is an intermittent process. Intermissions may be caused by an interaction between different phonon modes giving rise to a short break down of a mode. Due to such an intermittent behavior, we obtain — besides thermal noise — a 1/f noise component. Under equilibrium conditions, the 1/f noise term disappears. Under an applied electric field, the electrons are accelerated between collisions resulting in an additional 1/f noise component which can be compared with Hooge's relation. The predicted Hooge coefficient is α ≈ 3 ⋅ 10-3(τ off /τs)2 with τs being the mean electron phonon scattering time and τ off being the mean off-time ( = intermission). We also find 1/f fluctuations in the square of thermal noise suggesting that an applied current only probes 1/f fluctuations which are already present under equilibrium conditions.


2011 ◽  
Vol 84 (3) ◽  
Author(s):  
V. G. Tyuterev ◽  
S. V. Obukhov ◽  
N. Vast ◽  
J. Sjakste

2014 ◽  
Vol 5 (3) ◽  
pp. 982-992 ◽  
Author(s):  
M AL-Jalali

Resistivity temperature – dependence and residual resistivity concentration-dependence in pure noble metals(Cu, Ag, Au) have been studied at low temperatures. Dominations of electron – dislocation and impurity, electron-electron, and electron-phonon scattering were analyzed, contribution of these mechanisms to resistivity were discussed, taking into consideration existing theoretical models and available experimental data, where some new results and ideas were investigated.


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