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1979
DOI: 10.1063/1.2995671
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A Physicist's ABC on Plasma

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Cited by 32 publications
(45 citation statements)
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“…Thus, we can assume that a considerable part of plasma radiation is coupled to the target. Furthermore, hot laser-induced plasmas efficiently emit in the UV spectral range [43][44][45]59] where the reflection coefficient of materials is smaller as compared to IR and visible ranges. As a result, this additional heating can considerably increase the molten layer thickness.…”
Section: Plasma-assisted Ultradeep Ablationmentioning
confidence: 99%
See 1 more Smart Citation
“…Thus, we can assume that a considerable part of plasma radiation is coupled to the target. Furthermore, hot laser-induced plasmas efficiently emit in the UV spectral range [43][44][45]59] where the reflection coefficient of materials is smaller as compared to IR and visible ranges. As a result, this additional heating can considerably increase the molten layer thickness.…”
Section: Plasma-assisted Ultradeep Ablationmentioning
confidence: 99%
“…For singly ionized plasma (Z = 1), the photo-recombinative losses can be expressed as [22] In Equation (10), e is the unit charge, the electron and ion densities (ne, ni) are measured in cm −3 , and the electron temperature Te and ionization potential of carbon atoms IC are in eV. On the other hand, the radiation power densities of the bremsstrahlung and photo-recombination processes can be estimated as [59]: 34 2 0.5 brem Here the electron temperature is measured in Kelvins. Simulations have shown that Equations (10) and (12) give at Z = 1 the same recombinative radiation power.…”
Section: Plasma-assisted Ultradeep Ablationmentioning
confidence: 99%
“…This shock arises as a consequence of strong nonlinear upper-hybrid (UH) solitary waves which are driven via the beam instability by the ion beam. In this scenario, typical for collisionless shock generation (Artsimovich and Sagdeev, 1979), the shock front is formed by the dissipative process caused by particle heating, and the tail of the wave manifests itself as UH wave perturbations in the foot of the quasi-perpendicular shock. The dispersion law of the electrostatic UH wave (its wave potential is about 1 mc 2 ) at the foot of shock front is…”
Section: Stochastic Surfing Electron Acceleration At Galactic Shocksmentioning
confidence: 99%
“…the dispersion law of which is a typical condition for plasma modes induced by a beam (Artsimovich and Sagdeev, 1979), where ω p is the electron plasma frequency, and v f , v b are the speed of the front and beam respectively. In this situation electrons can be accelerated up to relativistic energies through the mechanism of surfing (Sagdeev et al, 1988).…”
Section: Stochastic Surfing Electron Acceleration At Galactic Shocksmentioning
confidence: 99%
“…The mechanical interpretation of an adiabatic process for an ideal gas is mentioned, for example, in [39,40] for k < 3, but is usually never considered in the presentation of thermodynamics in the courses of general and theoretical physics. Before proceeding to a consideration of an adiabatic process, we shall compare equilibrium canonical and microcanonical ensembles for bounded oscillator and symmetric Coulomb pair.…”
Section: Adiabatic and Other Ensembles Of Simple Dynamical Systemsmentioning
confidence: 99%