Volume 128, Number 1, October 2019
|Number of page(s)||5|
|Section||Condensed Matter: Electronic Structure, Electrical, Magnetic and Optical Properties|
|Published online||20 November 2019|
Simulation of temperature profile for the electron and the lattice systems in laterally structured layered conductors
1 Key Laboratory of Surface Physics, Institute of Nanoelectronic Devices and Quantum Computing, Key Laboratory of Micro and Nano Photonic Structures (Ministry of Education), Department of Physics, Fudan University Shanghai 200433, China
2 National Laboratory for Infrared Physics, Shanghai Institute of Technical Physics, The Chinese Academy of Sciences Shanghai 200083, China
3 Collaborative Innovation Center of Advanced Microstructures - Nanjing 210093, China
4 Terahertz Technology Research Center, NICT - Nukui-Kitamachi 4-2-1, Koganei, Tokyo, Japan
5 Department of Basic Science, The University of Tokyo - Komaba 3-8-1, Meguro-ku, Tokyo, 153-8902, Japan
6 School of Physical Science and Technology, ShanghaiTech University - Shanghai 201210, China
(a) firstname.lastname@example.org (corresponding author)
Received: 22 July 2019
Accepted: 15 September 2019
Electrons in operating microelectronic semiconductor devices are accelerated by locally varying a strong electric field to acquire effective electron temperatures nonuniformly distributing in nanoscales and largely exceeding the temperature of the host crystal lattice. The thermal dynamics of electrons and the lattice are hence nontrivial and its understanding at nanoscales is decisively important for gaining a higher device performance. Here, we propose and demonstrate that in layered conductors the nonequilibrium nature between the electrons and the lattice can be explicitly pursued by simulating the conducting layer by separating it into two physical sheets representing, respectively, the electron and the lattice subsystems. We take, as an example of simulating GaAs devices, a 35 nm thick, wide U-shaped conducting channel with 15 nm radius of curvature at the inner corner of the U-shaped bend, and find a remarkable hot spot to develop due to hot-electron generation at the inner corner. The hot spot in terms of the electron temperature achieves a significantly higher temperature and is of far sharper spatial distribution when compared to the hot spot in terms of the lattice temperature. A similar simulation calculation made on a metal (NiCr) narrow lead of similar geometry shows that a hot spot shows up as well at the inner corner, but its strength and the spatial profiles are largely different from those in semiconductor devices; viz., the amplitude and the profile of the electron system are similar to those of the lattice system, indicating quasi-equilibrium between the two subsystems. The remarkable difference between the semiconductor and the metal is interpreted to be due to the large difference in the electron specific heat, rather than the difference in the electron phonon interaction. This work will provide useful hints to a deeper understanding of the nonequilibrium properties of electrical conductors, through a simple and convenient method for modeling nonequilibrium layered conductors.
PACS: 73.63.-b – Electronic transport in nanoscale materials and structures / 44.05.+e – Analytical and numerical techniques / 05.70.Ln – Nonequilibrium and irreversible thermodynamics
© EPLA, 2019
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