2016
DOI: 10.1103/physrevb.94.134305
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Microscopic modeling of the effect of phonons on the optical properties of solid-state emitters

Abstract: Understanding the effect of vibrations in optically active nano systems is crucial for successfully implementing applications in molecular-based electro-optical devices, quantum information communications, single photon sources, and fluorescent markers for biological measurements. Here, we present a first-principles microscopic description of the role of phonons on the isotopic shift presented in the optical emission spectrum associated to the negatively charged silicon-vacancy color center in diamond. We use … Show more

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Cited by 27 publications
(31 citation statements)
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“…It is shown experimentally that different NV − center samples have an activation energy of 73 meV [8], which is close to the vibrational resonance frequency ω res = 65 meV. In our formalism, quasi-localized phonons can be phenomenologically modeled by a Lorentzian spectral density function of the form [16,35]…”
Section: Hamiltonianmentioning
confidence: 79%
“…It is shown experimentally that different NV − center samples have an activation energy of 73 meV [8], which is close to the vibrational resonance frequency ω res = 65 meV. In our formalism, quasi-localized phonons can be phenomenologically modeled by a Lorentzian spectral density function of the form [16,35]…”
Section: Hamiltonianmentioning
confidence: 79%
“…We note that these calculations inherently assume that the Franck-Condon principles hold for the optical transitions, i.e., the optical transition dipole moment is independent from the ionic movements. This is a valid approximation for the optical transition between the triplets of NV center in diamond but it does not necessarily holds for all types of vibrations and solid state defect quantum bits, in which the Herzberg-Teller interaction is considerable 216 . We showed above that the fluorescence of the singlets of NV center in diamond does not follow the Franck-Condon principles either, and one should use polaronic wave functions in the calculation of the optical spectrum.…”
Section: F Radiative and Non-radiative Rates: A Complete Theory On Tmentioning
confidence: 99%
“…where ∆ = ω eg − ω L is the detuning from the bare transition frequency ω eg and Ω is the optical Rabi frequency. The g k = λ e,k − λ g,k [36] denote the effective electron-phonon coupling constants, which arise from the different deformation potentials, λ e,k and λ g,k , in the ground and the excited state.…”
Section: Optical Coherence For Orbital States Of Color Centersmentioning
confidence: 99%
“…( 6) we see that the dephasing rate γ(t), and thus the degree of NM, depends only on the SDF, J(ω), and the temperature T . In the case of color centers or other solid-state emitters, information about the SDF can be obtained from the photoluminescence (PL) spectrum [36,38], where the coupling to the phonons both reduces the bare resonance (zero-phonon line) and leads to additional phonon-sidebands. The experimental PL spectrum of the SiV − center exibits an isotopic shift feature in the prominent and narrow phonon sideband [38].…”
Section: Phonon Spectral Density and Dephasing Ratementioning
confidence: 99%