2021
DOI: 10.1016/j.physb.2021.412982
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Study of coulomb drag with the effect of local field correction and dielectric medium

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Cited by 3 publications
(1 citation statement)
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“…where χ 0 (q, ω) and χ(q, ω) are the dynamic density response functions of noninteracting and interacting systems, respectively, and v q = 8π/q 2 is the long-range Coulomb repulsion (Rydberg atomic units are used). The LFC encodes the structure of effective electron-electron interaction and is crucial for the understanding of many experimental phenomena, exemplified by plasmon [11,20], Coulomb and spin-Coulomb drag effects [21,22], electrical and thermal conductivities [23,24], stopping power [25,26], and energy transfer rates [27]. In the timedependent density functional theory (TDDFT) [19,28], the so-called XC kernel, K xc (q, ω) = −v q G(q, ω), is typically used as an input for ab-inito calculations of groundstate energies and electronic spectra in real materials.…”
mentioning
confidence: 99%
“…where χ 0 (q, ω) and χ(q, ω) are the dynamic density response functions of noninteracting and interacting systems, respectively, and v q = 8π/q 2 is the long-range Coulomb repulsion (Rydberg atomic units are used). The LFC encodes the structure of effective electron-electron interaction and is crucial for the understanding of many experimental phenomena, exemplified by plasmon [11,20], Coulomb and spin-Coulomb drag effects [21,22], electrical and thermal conductivities [23,24], stopping power [25,26], and energy transfer rates [27]. In the timedependent density functional theory (TDDFT) [19,28], the so-called XC kernel, K xc (q, ω) = −v q G(q, ω), is typically used as an input for ab-inito calculations of groundstate energies and electronic spectra in real materials.…”
mentioning
confidence: 99%