Investigating the role of electron—phonon scattering in the measurement of photoelectric thresholds

1975 ◽  
Vol 6 (4) ◽  
pp. 321-323
Author(s):  
I. Abbati ◽  
L. Braicovich ◽  
B. De Michelis ◽  
A. Fasana
1992 ◽  
Vol 68 (8) ◽  
pp. 1156-1159 ◽  
Author(s):  
J. F. DiTusa ◽  
K. Lin ◽  
M. Park ◽  
M. S. Isaacson ◽  
J. M. Parpia

2017 ◽  
Vol 19 (32) ◽  
pp. 21714-21721 ◽  
Author(s):  
Long Cheng ◽  
Qing-Bo Yan ◽  
Ming Hu

The layered metal oxide PdCoO2 is of fundamental interest in solid-state physics due to its unique nature as a two-dimensional electron gas.


2012 ◽  
Vol 730-732 ◽  
pp. 159-163
Author(s):  
Teresa M. Seixas ◽  
Manuel A. Salgueiro da Silva ◽  
Hans F. Braun ◽  
Georg Eska

We report on a comparative study of thermoelectric power measurements (S(T)) in ferrimagnetic Gd4(Co1-xAx)3 compounds with A = Cu, Pt, in the temperature range 8 K – 300 K. Whereas in Gd4Co3S(T) is always negative, for x > 0 the substitution of Co for Cu/Pt gives rise to the appearance of a low temperature positive maximum in S(T) at around 30 K. Based on our previous study of Gd4(Co1-xCux)3 compounds, we argue that this maximum in S(T) originates from electron-magnon scattering and is sensitive to electron band structure changes resulting from the substitution of Co for Cu/Pt and the accompanying reduction in the ratio between the electron-magnon and the electron-phonon scattering strengths. The decreasing role of Co 3d electrons with the progressive substitution of Co for Cu/Pt, evidenced by a strong reduction in the spin disorder resistivity and the Co magnetic moment, is seen to be crucial for the existence of such low temperature maximum in S(T) for x > 0. It is seen that the substitution of Co for Pt leads to higher values of the amplitude and temperature of the positive maximum in S(T) than the substitution of Co for Cu.


2014 ◽  
Vol 1661 ◽  
Author(s):  
Jawaher Al-Otaibi ◽  
Gyaneshwar P. Srivastava

ABSTRACTIn this work we present a theoretical study of the transport coefficients of n-type PbTe. The electronic transport coefficients are calculated using the isotropic-nearly-free-electron approximation, including the effect of band non-parabolicity on electron-phonon scattering. The lattice thermal transport coefficient is computed by employing the isotropic continuum model for the dispersion relation for acoustic as well as optical phonon branches, an isotropic anharmonic continuum model for crystal anharmonicity, and the single-mode relaxation time scheme. The role of transverse optical (TO) phonon modes in anharmonic interactions will be discussed in detail.


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