2012
DOI: 10.1063/1.4721495
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On conversion of luminescence into absorption and the van Roosbroeck-Shockley relation

Abstract: Articles you may be interested inQuasi-Fermi level splitting and sub-bandgap absorptivity from semiconductor photoluminescence Observation of room temperature optical absorption in InP/GaAs type-II ultrathin quantum wells and quantum dots

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Cited by 69 publications
(48 citation statements)
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“…On the other hand, it is also useful to evaluate the perovskite behavior in the ideal bimolecular limit, since, owed to their peculiar optical properties of these systems, we can expect unusually small recombination rates and extra‐long radiative lifetimes. To the aim, we used our ab‐initio band structure calculations in combinations with the band‐to‐band recombination rate calculated according to the Van Roosbroeck‐Shockley theory . In Figure , the recombination properties as a function of the injected electron‐hole population n at room temperature are reported.…”
Section: Resultsmentioning
confidence: 99%
“…On the other hand, it is also useful to evaluate the perovskite behavior in the ideal bimolecular limit, since, owed to their peculiar optical properties of these systems, we can expect unusually small recombination rates and extra‐long radiative lifetimes. To the aim, we used our ab‐initio band structure calculations in combinations with the band‐to‐band recombination rate calculated according to the Van Roosbroeck‐Shockley theory . In Figure , the recombination properties as a function of the injected electron‐hole population n at room temperature are reported.…”
Section: Resultsmentioning
confidence: 99%
“…fu and fu are the Fermi-Dirac distributions of charge carries in the emitter material. The absorption rate σ(ω) is calculated under the condition that the upper state is empty and the lower state is full, and thus is uniquely defined by the available charge carrier DOS inside the material and by the transition selection rules imposed by momentum conservation [68,69]. Accordingly, the material absorption rate can be tailored by engineering the electron DOS, for example, via electron confinement effects.…”
Section: The Role Of Electron and Photon Densities Of States And The mentioning
confidence: 99%
“…Furthermore, most materials do not emit as blackbodies, and an energy-dependent "gray body" factor typically needs to be introduced to account for intrinsic material properties, which can be tailored by material engineering. For example, for a gray body semiconductor exhibiting an electronic bandgap and thus emitting photons carrying chemical potential, the emission rate is typically calculated via the van Roosbroeck-Shockley equation: [67][68][69]. This equation is valid for emitters exhibiting a quasi-thermal equilibrium within their respective electronic bands, including excited and ground state electrons, and also for µγ.…”
Section: The Role Of Electron and Photon Densities Of States And The mentioning
confidence: 99%
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“…with the spontaneous emission spectrum S ω, α(ω) calculated with a nonequilibrium Kubo-Martin-Schwinger relation as given, e.g., in Reference [35] using the absorption coefficient α(ω) proportional to the reciprocal periodicity length −1 . Numerically we find that the spontaneous emission current is below 1 A·cm −2 for QD densities up to 5 × 10 11 cm −2 and therefore negligible for the QD model under study.…”
Section: Setupmentioning
confidence: 99%