2020
DOI: 10.1007/s11433-020-1550-4
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Anharmonic multi-phonon nonradiative transition: An ab initio calculation approach

Abstract: Nonradiative carrier recombination at semiconductor deep centers is of great importance to both fundamental physics and device engineering. In this letter, we provide a revised analysis of K. Huang's original nonradiative multi-phonon (NMP) theory with ab initio calculations. First, we identify at first-principle level that Huang's concise formula gives the same results as the matrix based formula, and Huang's high temperature formula provides an analytical expression for the coupling constant in Marcus theory… Show more

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Cited by 34 publications
(19 citation statements)
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“…First-principles calculations have obtained great success in the research of GaN-based semiconductors 24,28,29,38,39 . In this work, we theoretically demonstrated by first-principles calculations that in GaN-based semiconductors, the 4 | 8 configuration is more energetically favorable than the wurtzite configuration after reducing the dimensions from bulk to 2D structures.…”
Section: Introductionmentioning
confidence: 99%
“…First-principles calculations have obtained great success in the research of GaN-based semiconductors 24,28,29,38,39 . In this work, we theoretically demonstrated by first-principles calculations that in GaN-based semiconductors, the 4 | 8 configuration is more energetically favorable than the wurtzite configuration after reducing the dimensions from bulk to 2D structures.…”
Section: Introductionmentioning
confidence: 99%
“…It is ascribed to the essence that the distortion of the Pb-Br bond is harder than that of the Pb-I bond determined by the bond length, which is reflected by the coupling parameter α as listed in Table I. We have noticed that the effective phonon modes and relaxation energy could be obtained from the first-principles calculations [39][40][41], gaining the more accurate evaluations for HR factors. Our results will also provide an important theoretical reference for these calculations.…”
Section: Resultsmentioning
confidence: 99%
“…[51] It should be noted that our electron-phonon calculations are considered within the harmonic approximation, anharmonic multiphonon process is beyond of the scope. [52] The total current for one spin channel can be expressed the as sum of two terms el in…”
Section: Theoretical Methodsmentioning
confidence: 99%
“…[ 51 ] It should be noted that our electron–phonon calculations are considered within the harmonic approximation, anharmonic multiphonon process is beyond of the scope. [ 52 ] The total current for one spin channel can be expressed the as sum of two terms Iσ=Ielσ+Iinσ (σ = up, down) and the spin‐resolved pure elastic current can be described by the Landauer formula Ielσ=G02edε[nnormalf(εμnormalL)nnormalf(εμnormalR)]Tσ(ε) where n f (ε) denotes to the Fermi–Dirac distribution function and μ L/R represents the chemical potential of the left/right electrode. The transmission coefficient can be given by T σ (ε) = Tr[ G r Γ L G a Γ R ] σ , here G r/a is the unperturbed retarded/advanced green function, Γ L/R is the broadening function of the left/right.…”
Section: Theoretical Methodsmentioning
confidence: 99%