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Such electron heating requires very high frequencies (tens to hundreds of gigahertz), such as produced by free-electron lasers and gyrotron tubes.
Preferential electron heating in the flow bursts is also statistically confirmed.
The major process during the laser-target interaction is the electron heating by the laser field.
However, time-varying electric fields could also play a role in beam production and electron heating.
The optimum polarization was applied to the electron heating experiment of JT-60U.
This result well corresponds to the electron heating in highly ordered pyrolytic graphite films reported in Ref. [21].
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Monte Carlo (MC) algorithm allows to vary electron heat conduction κ and hence the heat diffusion coefficient χ.
The fast temperature-dependent electron heat conduction leads to the redistribution of the deposited energy within the film.
The utilization of double-resonance energy filter leads to increased power output while decreased efficiency for the electron heat engine device.
Theoretical modeling for a microscopic ESE (energy selective electron) heat engine with double-resonance energy filters is performed in this paper.
Detectors based on a quantum well (QW) are a good choice, because the momentum quantization in the QW growth direction allows for a significant reduction of the 2D electron heat capacity.
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