scholarly journals Nonequilibrium distribution functions of nucleons in relativistic nucleus-nucleus collisions

2013 ◽  
Vol 16 (1) ◽  
pp. 13201 ◽  
Author(s):  
Anchishkin ◽  
Naboka ◽  
Cleymans
2021 ◽  
Author(s):  
Azuma Suzuki

Abstract The nonequilibrium distribution functions (NDF) for the trap states in the mobility-gap under photo illumination and zero bias voltage are derived by the constructed self-consistent drift-diffusion simulator consisted of the Poisson equation and current continuity equations for hydrogenated amorphous silicon (a-Si:H). As for the temperature dependence of the NDF, we find that the values of the NDF decrease with increasing temperature (the negative temperature dependence) in the energy region near the conduction band for p-type a-Si:H. That is the reverse of the temperature dependence of the equilibrium distribution functions (EDF) for the trap states in the mobility-gap. Furthermore, we show that the new physical characteristic is applicable to the explanation of the temperature characteristic of the photoconductivity caused by the electron hopping in the conduction band tail for a-Si:H. The photoconductivity of a-Si:H decreases with increasing temperature, which is called the thermal quenching (TQ). We show that the TQ observed in a low temperature around 200K for p-type a-Si:H can be explained by the electron hopping model with the p-type NDF having the negative temperature dependence.


1980 ◽  
Vol 45 (2) ◽  
pp. 124-125 ◽  
Author(s):  
Denis J. Evans ◽  
William G. Hoover ◽  
Anthony J. C. Ladd

1995 ◽  
Vol 09 (08) ◽  
pp. 991-1000
Author(s):  
D.Y. XING ◽  
J. YANG ◽  
C.S. TING

The closed time path Green’s function method is used to derive the nonequilibrium distribution functions of acoustic phonons and excitations of hot electrons, renormalized by the electron-phonon interaction in the random phase approximation, and to calculate the power dissipation of hot electrons. It is shown that the energy loss channel of hot electrons would vanish unless a relaxation rate corresponding to the decay of one acoustic phonon into two or more bare acoustic phonons via the anharmonic interaction is explicitly included in the phonon propagator. The effect due to the anharmonic interaction on the energy loss rate of hot electrons has also been studied.


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