2009
DOI: 10.1103/physrevb.80.165104
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Light scattering in a phonon gas

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Cited by 17 publications
(16 citation statements)
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“…It is hence likely that it originates from a Raman scattering process occurring in the SiN core. Such broadband Raman scattering has been ascribed to breaking of momentum selection rules due to disorder in the amorphous material, and photon-phonon coupling due to thermal fluctuations [ 20 , 21 , 22 ]. A detailed study of the behavior of such a Raman scattering process in a guiding structure is outside the scope of this paper.…”
Section: Resultsmentioning
confidence: 99%
“…It is hence likely that it originates from a Raman scattering process occurring in the SiN core. Such broadband Raman scattering has been ascribed to breaking of momentum selection rules due to disorder in the amorphous material, and photon-phonon coupling due to thermal fluctuations [ 20 , 21 , 22 ]. A detailed study of the behavior of such a Raman scattering process in a guiding structure is outside the scope of this paper.…”
Section: Resultsmentioning
confidence: 99%
“…Observations of second sound were made with heat pulse experiments in 3 He (between 0.42 and 0.58 K) (11), in Bi (between 1.2 and 4 K) (12), and in NaF (between 11 and 14.5 K) (13,14). The reported occurrence of second sound in SrTiO 3 at 30 to 40 K (15,16) is in dispute, as others argued that the attribution of the low-frequency doublet in the Brillouin spectra to second sound was not supported by the observations (17,18). Computational work indicated that the temperature window for the phonon hydrodynamics regime is much wider in graphene ( 9) and other twodimensional (2D) materials (19) because of strong normal scattering involving the flexural mode.…”
mentioning
confidence: 99%
“…As mentioned by Lee et al [18], these experiments can be broadly distinguished as two different methods: (a) Heat-pulse experiments and (b) Light scattering experiments. In literature, both the heat-pulse experiments [16,94,[96][97][98][99][100][101][102] and the light scattering methods [26,95,[103][104][105][106][107][108][109] have been proved to be effective to detect second sound in solids. In a standard heat pulse experiment [16,18,99], a heat pulse is generated at the one end of the sample and the temporal response of temperature is monitored at the opposite end whereas light scattering techniques measure the local change of dielectric constants due to the propagation of second sound.…”
Section: Experimental Methods and Observationsmentioning
confidence: 99%
“…However, it was found that SrTiO 3 possesses strong Normal scattering due to strongly anharmonic soft transverse optical phonons [113]. Motivated by this idea, Koreeda et al [26,108] explored low-frequency light scattering experiments without employing a thermal fluctuation field to investigate the propagation of second sound in SrTiO 3 . They observed an underdamped second sound for SrTiO 3 below 40 K [26].…”
Section: Experimental Methods and Observationsmentioning
confidence: 99%
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