2018
DOI: 10.1103/physrevb.97.094308
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Interaction between confined phonons and photons in periodic silicon resonators

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Cited by 4 publications
(2 citation statements)
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“…Second, the mode line shape is irreversible; that is, when the temperature rises to 1000 K and goes back down, the E2High mode displays completely different line shapes than the ones displayed when heating the sample. As the average grain size is too high to confine phonons and cause line broadening, [ 30 ] the observed behavior of the Raman line shape can only be due to the displacement of the 0.25emE2High mode resonance along the ridge of the two‐phonon DOS when the temperature changes and to a marked effect of thermal annealing on the two‐phonon DOS. A numerical technique for extracting from the recorded Raman spectra the two‐phonon DOS of the measured samples before and after thermal annealing is presented below.…”
Section: Resultsmentioning
confidence: 99%
“…Second, the mode line shape is irreversible; that is, when the temperature rises to 1000 K and goes back down, the E2High mode displays completely different line shapes than the ones displayed when heating the sample. As the average grain size is too high to confine phonons and cause line broadening, [ 30 ] the observed behavior of the Raman line shape can only be due to the displacement of the 0.25emE2High mode resonance along the ridge of the two‐phonon DOS when the temperature changes and to a marked effect of thermal annealing on the two‐phonon DOS. A numerical technique for extracting from the recorded Raman spectra the two‐phonon DOS of the measured samples before and after thermal annealing is presented below.…”
Section: Resultsmentioning
confidence: 99%
“…Unlike for c-Si, in the case of SiNSs, the abovementioned k = 0 selection rule gets relaxed, first reported by Richter et al [71] and Campbell and Fauchet [72] and later on validated by many others. [37,41,66,[73][74][75][76][77][78][79][80] As a consequence of momentum relaxation, phonons other than the zone centered ones, governed by phonon dispersion relation, also contribute in a crystallite of finite dimension. This results in a change in the first order Raman spectrum, which is typically Lorentzian for crystalline materials.…”
Section: Origin Of Asymmetric Raman Line Shape In Siliconmentioning
confidence: 99%