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Taking into account electronic velocity spread, and cavity wall resistivity and basing on single-mode approximation, the optimized design and simulation of beam-wave interaction of a 170 GHz MW corrugated coaxial-gyrotron have be fulfilled.
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The EPW v4 program can be used to compute electron and phonon self-energies, linewidths, electron phonon scattering rates, electron phonon coupling strengths, transport spectral functions, electronic velocities, resistivity, anisotropic superconducting gaps and spectral functions within the Migdal Eliashberg theory.
where D k = 2/(2π)2 is the density of electronic states in k-space, v → ( k → ) = v F is the electron velocity, and g ( k → ) is the distribution function.
The mathematical expressions presented here apply strictly in the high-velocity, electronic excitation domain.
This equation states that the current is the product of the electronic charge (q), a velocity (v), and (N_{text{c}}) the density of available charge carriers in the metal semiconductor interface.
For the same electronic energy loss, the velocity of the incident ion could affect the energy and spatial distribution of excited electrons, and therefore effectively modify the diameter of the ion track.
Good agreement between the calculated projected ranges and the experimental data in the energy range of 10 1000 keV gives use in the range-projection equations the nuclear energy losses, determined with the first-principles potentials, and the velocity proportional electronic stopping powers by Land and Brennan (LB).
The maximal angular velocity of electronic gyrometry was 2000°/s and the sensitivity was 0.5 mV/°/s.
We model electronic stopping by a velocity-proportional friction force F=n k v, where n is the atomic number density of Au and v is the atom velocity.
Good agreement between the calculated projected ranges and the experimental data in the energy range of 10 to 1000 keV gives use in the range projection equations the nuclear stopping powers, determined with first-principles potentials, and the velocity-proportional electronic stopping powers by Land and Brennan (LB).
Substituting for electronic specific heat and Fermi velocity in Equation 1 leads to the relationship: (2).
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