2023
DOI: 10.1103/physrevmaterials.7.024006
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First-principles study of luminescence in hexagonal boron nitride single layer: Exciton-phonon coupling and the role of substrate

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Cited by 10 publications
(11 citation statements)
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“…To comprehend excitonic thermalization, we employ a similar fitting approach, as demonstrated by Cassabois et al, to the falling edge of the spectra, employing an exponential Boltzmann factor with an effective temperature T eff . From the plot depicting T eff against the lattice temperature T lat (see Figure ), it becomes evident that the excitons thermalize with the crystal beyond 25 K. This observation aligns with a recently reported case concerning emission spectra from monolayer h-BN …”
Section: Resultssupporting
confidence: 89%
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“…To comprehend excitonic thermalization, we employ a similar fitting approach, as demonstrated by Cassabois et al, to the falling edge of the spectra, employing an exponential Boltzmann factor with an effective temperature T eff . From the plot depicting T eff against the lattice temperature T lat (see Figure ), it becomes evident that the excitons thermalize with the crystal beyond 25 K. This observation aligns with a recently reported case concerning emission spectra from monolayer h-BN …”
Section: Resultssupporting
confidence: 89%
“…Hence, to speed up the convergence, we interpolated the phonon energies on a dense q grid of 60 × 60 × 1. A smooth Fourier interpolation (“double-grid approach”) can then be used to interpolate the electronic energies at k + q . , We therefore fixed the course grid at 12 × 12 × 1 and converged the quasi-particle energy gap for a variety of dense q grids (see Figure S16 in the SI for the quasiparticle gap convergence with respect to q -grids).…”
Section: Computational Methodologymentioning
confidence: 99%
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“…Beside a direct-gap opening of 2.8 eV at the K -point of the first BZ, quasi-particle (QP) corrections to the Kohn–Sham band structure also induce a direct-indirect band gap transition due to a nearly free-electron conduction state at Γ descending below the bottom of the conduction band at K . Our findings are consistent with previous works , (see the SI for additional details). The same behavior is observed when excitonic effects are included through the BSE: as can be seen from the excitonic band structure in Figure a, the energy of the indirect exciton at q = K ( E K (1) ) is 30 meV below the energy of the direct exciton ( E Γ (1) ).…”
supporting
confidence: 94%
“…At this point, it is important to note that recent first-principles MBPT calculations have suggested that the interaction with the substrate, which is always present in real experiments, pushes the nearly free-electron band at Γ above the bottom of the conduction band at K , making m-BN a direct gap semiconductor . Under these conditions, phonon satellites below the QP peak should be essentially absent, in contrast with experimental observations. , Based on our analysis of the exc-ph coupling, a possible explanation for the phonon satellites observed in the experimental spectra is that m-BN is actually a multivalley semiconductor consisting of two nearly degenerate exciton valleys, namely, E Γ (1) and E K (2) .…”
mentioning
confidence: 59%