Publication | Closed Access
Plasma dynamics in a hollow cathode triggered discharge with the influence of fast electrons on ionization phenomena and EUV emission
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Citations
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References
2008
Year
EngineeringIonization KineticsPlasma SciencePlasma PhysicsPlasma ElectronicsIonization Wave PropagationPlasma TheoryPlasma SimulationPlasma ComputationMagnetohydrodynamicsPlasma ConfinementPhysicsApplied Plasma PhysicAtomic PhysicsLaboratory Plasma PhysicsPlasma ApplicationHollow CathodeElectron BeamApplied PhysicsFast ElectronsGas Discharge PlasmaPlasma Dynamics
The 2D computational code Z* is used to simulate physical phenomena in a hollow cathode triggered low-pressure capillary discharge at different phases of the process: electron beam generation, formation of a channel by an ionization wave and discharge dynamics together with ionization kinetics and plasma emission, particularly in the EUV band, which is interesting for applications. Runaway electrons in a gas-filled capillary discharge with a hollow cathode play an important role both in ionization wave propagation and in ionization of multicharged ions in a discharge plasma. The electron beam prepares a tight ionized channel. The fast electrons shift the ionization equilibrium in the discharge plasma, increasing the EUV emission from the relatively low-temperature plasma of argon or xenon. At the ionization wave stage, the electron flow is simulated in an electron-hydrodynamic model. At the discharge stage, the plasma is described by the radiative magnetohydrodynamics with ionization kinetics and radiation transfer. The universal method for calculation of cross-sections of electron–ion inelastic impact processes in a plasma of multicharged ions in a wide range of plasma parameters is realized in computational code on the basis of the Hartree–Fock–Slater quantum-statistical model of a self-consistent field for the average atom and the distorted wave approximation.
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