Search results for "exciton-phonon coupling"

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Exciton-Phonon Coupling in the Ultraviolet Absorption and Emission Spectra of Bulk Hexagonal Boron Nitride

2018

We present an \textit{ab initio} method to calculate phonon-assisted absorption and emission spectra in the presence of strong excitonic effects. We apply the method to bulk hexagonal BN which has an indirect band gap and is known for its strong luminescence in the UV range. We first analyse the excitons at the wave vector $\overline{q}$ of the indirect gap. The coupling of these excitons with the various phonon modes at $\overline{q}$ is expressed in terms of a product of the mean square displacement of the atoms and the second derivative of the optical response function with respect to atomic displacement along the phonon eigenvectors. The derivatives are calculated numerically with a fin…

Materials sciencePhononExciton: Physics [G04] [Physical chemical mathematical & earth Sciences]Ab initioFOS: Physical sciencesGeneral Physics and Astronomy01 natural sciencesMolecular physicsCondensed Matter::Materials Sciencephonon-assisted luminescenceMesoscale and Nanoscale Physics (cond-mat.mes-hall)0103 physical sciencesEmission spectrum010306 general physicsAbsorption (electromagnetic radiation)Condensed Matter - Materials ScienceCondensed Matter - Mesoscale and Nanoscale PhysicsMaterials Science (cond-mat.mtrl-sci)Condensed Matter::Mesoscopic Systems and Quantum Hall EffectCoupling (probability): Physique [G04] [Physique chimie mathématiques & sciences de la terre]indirect absorptionDirect and indirect band gapsLuminescenceexciton-phonon couplingPhysical Review Letters
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Time-dependent screening explains the ultrafast excitonic signal rise in 2D semiconductors

2020

We calculate the time evolution of the transient reflection signal in an MoS$_2$ monolayer on a SiO$_2$/Si substrate using first-principles out-of-equilibrium real-time methods. Our simulations provide a simple and intuitive physical picture for the delayed, yet ultrafast, evolution of the signal whose rise time depends on the excess energy of the pump laser: at laser energies above the A- and B-exciton, the pump pulse excites electrons and holes far away from the K valleys in the first Brillouin zone. Electron-phonon and hole-phonon scattering lead to a gradual relaxation of the carriers towards small $\textit{Active Excitonic Regions}$ around K, enhancing the dielectric screening. The acc…

ab-initio many-body perturbation theoryMaterials scienceExciton: Physics [G04] [Physical chemical mathematical & earth Sciences]General Physics and AstronomyFOS: Physical sciences02 engineering and technology010402 general chemistry01 natural sciencesSignalCondensed Matter::Materials ScienceMonolayerGeneral Materials ScienceCondensed Matter - Materials Sciencebusiness.industryGeneral EngineeringTime evolutionMaterials Science (cond-mat.mtrl-sci)Computational Physics (physics.comp-ph)021001 nanoscience & nanotechnologytime-dependent spectroscopy0104 chemical sciencesReflection (mathematics)Semiconductor: Physique [G04] [Physique chimie mathématiques & sciences de la terre]OptoelectronicsTransient (oscillation)0210 nano-technologybusinessUltrashort pulsePhysics - Computational Physicsexciton-phonon couplingPhysics - OpticsOptics (physics.optics)
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