Hot Electron Energy Relaxation in Gallium Nitride

1999 ◽  
Vol 176 (1) ◽  
pp. 369-372 ◽  
Author(s):  
N. M. Stanton ◽  
P. Hawker ◽  
A. J. Kent ◽  
T. S. Cheng ◽  
C. T. Foxon
1989 ◽  
Vol 4 (10) ◽  
pp. 852-857 ◽  
Author(s):  
N Balkan ◽  
B K Ridley ◽  
M Emeny ◽  
I Goodridge

2008 ◽  
Vol 23 (7) ◽  
pp. 075048 ◽  
Author(s):  
A Matulionis ◽  
J Liberis ◽  
E Šermukšnis ◽  
J Xie ◽  
J H Leach ◽  
...  

2020 ◽  
Vol 34 (32) ◽  
pp. 2050322
Author(s):  
A. L. Vartanian ◽  
A. L. Asatryan ◽  
A. G. Stepanyan ◽  
K. A. Vardanyan ◽  
A. A. Kirakosyan

The energy relaxation of hot electrons is proposed based on the spin–orbit (SO) interaction of both Rashba and Dresselhaus types with the effect of hot phonons. A continuum theory of optical phonons in nanowires taking into account the influence of confinement is used to study the hot-electron energy relaxation. The energy relaxation due to both confined (CO) and interface (IO) optical phonon emission on nanowire radius, electrical field strength, parameters of SO couplings and electron temperature is calculated. For considered values of the nanowire radius as well as other system parameters, scattering by IO phonons prevails over scattering by CO phonons. The presence of an electric field leads to the decrease of power loss in transitions between states with the same spin quantum numbers. With the increase of the electric field strength, the influence of the Dresselhaus SO interaction on the energy relaxation rate decreases. The effect of SO interaction does not change the previously obtained increasing dependence of power loss on electron temperature. The sensitivity of energy relaxation to the electric field also through the Rashba parameter allows controlling the rate of energy by electric field.


2004 ◽  
Vol 19 (4) ◽  
pp. S440-S442 ◽  
Author(s):  
C E Martinez ◽  
N M Stanton ◽  
A J Kent ◽  
M L Williams ◽  
I Harrison ◽  
...  

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