2011
DOI: 10.1063/1.3600533
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Stopping power for a charged particle moving through three-dimensional nonideal finite-temperature electron gases

Abstract: We investigate the interaction of a charged particle with nonideal 3D electron gases by using the quantum hydrodynamic (QHD) theory. The stopping power for a nonideal electron gas at a finite-temperature has been theoretically analyzed and numerically calculated. In our calculation, the impact of nonideality and temperature on stopping power is stressed and clearly presented. The QHD dielectric function is obtained and compared to random-phase approximation result. It is shown that the QHD theory can properly … Show more

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Cited by 8 publications
(6 citation statements)
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References 30 publications
(33 reference statements)
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“…The projectile position is shown as a green triangle. We see the electron wake, predicted in HEG, is significantly distorted by the background atoms [68,69].…”
Section: Theory Stopping Power Modelsmentioning
confidence: 78%
“…The projectile position is shown as a green triangle. We see the electron wake, predicted in HEG, is significantly distorted by the background atoms [68,69].…”
Section: Theory Stopping Power Modelsmentioning
confidence: 78%
“…In what follows the frictional coefficient is obtained from our previous work. 28 We take the incident particle as a proton and assume that the charged particle is projected from z ¼ 0 at t ¼ 0. For future use a dimensionless variable r 0 ¼ ð3Z i =4pn 0 a 3 B Þ 1=3 is employed as a function of the EG density in equilibrium n 0 and the atomic number Z i .…”
Section: Numerical Resultsmentioning
confidence: 99%
“…In order to compare the wake potentials between nonlinear and linear QHD methods, we briefly describe the linearized wake potential by adopting our previous work. 28 In our previous work, by employing u e (R, t) ¼ u e1 (R, t) and n e (R, t) ¼ n 0 þ n e1 (R, t) with the 3D coordinate vector R, the linearized QHD equations about n e1 (R, t) and u e1 (R, t) can be obtained, where u e1 (R, t) and n e1 (R, t) represent the firstorder perturbed values of velocity and density. With a timespace Fourier transform in the linearized equations, then after a process of simplifying and arranging the equations, a 3D linear wake potential in cylindrical coordinate system with R ¼ {q, u, z} is given as…”
Section: Nonlinear Quantum Hydrodynamic Modelmentioning
confidence: 97%
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“…(2) and (3) are the frictional forces with γ and τ w obtained from our previous work (Zhang et al, 2011a).…”
Section: Quantum Hydrodynamic Modelmentioning
confidence: 99%