1998
DOI: 10.1103/physreva.57.200
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Velocity-dependent screening in metals

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Cited by 79 publications
(72 citation statements)
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“…Many different physical processes contribute to the electronic stopping: ionization of the target atoms, excitation of electrons into the conduction band, collective electronic excitations such as plasmons, etc. [89][90][91][92][93][94][95][96][97][98][99][100][101][102] Electronic stopping dominates at high ion energies ͑see Fig. 2͒.…”
Section: A Production Of Defects In Bulk Targetsmentioning
confidence: 99%
“…Many different physical processes contribute to the electronic stopping: ionization of the target atoms, excitation of electrons into the conduction band, collective electronic excitations such as plasmons, etc. [89][90][91][92][93][94][95][96][97][98][99][100][101][102] Electronic stopping dominates at high ion energies ͑see Fig. 2͒.…”
Section: A Production Of Defects In Bulk Targetsmentioning
confidence: 99%
“…It is important to stress that other choices of screening functions from Ref. 13 like, for instance, the single-zeta type, could enlarge the mean energy loss straggling due to the Coulomb explosion and the Coulomb heating effect value as well.…”
Section: ͑8͒mentioning
confidence: 99%
“…The angle between the molecular axis and the motion direction is chosen randomly, as well as the projectile initial position along the transverse channel plane. The interaction between the fragments of the H 2 + molecule was modeled using three different potentials: ͑i͒ a pure Coulomb potential; ͑ii͒ a Yukawa potential with a dynamic screening function according to the Arista and Lifschitz approach 13 ͑screening length of about 4 a . u. for the present case͒; and ͑iii͒ a wake-type potential, whose target dielectric properties were described by a Mermim dielectric function ͑using an electron radius of r s =2 a.u.͒.…”
Section: ͑2͒mentioning
confidence: 99%
“…[16]): a) the Coulomb potential, that describes the potential induced by a moving point charge in vacuum; b) the Bohr potential, that describes a potential produced by a external point charge immersed in a homogenous electron gas. The screening parameter (α i ) can be obtained either from the Debye screening length [17] or from the generalization of the Friedel sum rule for finite velocities derived by Lifschitz and Arista [18]; c) the single-zeta potential, that describes the potential due a projectile carrying one or two bound electrons (n i = 1, 2) in hydrogen-like 1s orbitals.…”
Section: Modelmentioning
confidence: 99%