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Volumn 94, Issue 10, 2009, Pages

Optimized optical generation and detection of superlattice acoustic phonons

Author keywords

[No Author keywords available]

Indexed keywords

ACOUSTICS; ELECTROMAGNETIC WAVE EMISSION;

EID: 62549124583     PISSN: 00036951     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.3097244     Document Type: Article
Times cited : (20)

References (16)
  • 5
    • 0141564675 scopus 로고    scopus 로고
    • 0740-3224 10.1364/JOSAB.19.003028.
    • O. Matsuda and O. B. Wright, J. Opt. Soc. Am. B 0740-3224 10.1364/JOSAB.19.003028 19, 3028 (2002).
    • (2002) J. Opt. Soc. Am. B , vol.19 , pp. 3028
    • Matsuda, O.1    Wright, O.B.2
  • 12
    • 0001940305 scopus 로고
    • in, edited by M. Cardona and G. Güntherodt (Springer, Heidelberg),.
    • B. Jusserand and M. Cardona, in Light Scattering in Solids V, edited by, M. Cardona, and, G. Güntherodt, (Springer, Heidelberg, 1989), p. 49.
    • (1989) Light Scattering in Solids v , pp. 49
    • Jusserand, B.1    Cardona, M.2
  • 15
    • 62549094337 scopus 로고    scopus 로고
    • The calculated spectra were obtained using Eqs. (1) and (2) of Ref. together with the continuum model for the eigenmodes of the sample. The enhancement factor is defined as in the experiment, i.e. the ratio between the maximum peak intensity and the average of the generation peak intensity over the other seven detuning conditions. In the case of full optical decoupling, the generation (photoelastic) constant in the probe (pump) SL was taken as 0.
    • The calculated spectra were obtained using Eqs. (1) and (2) of Ref. together with the continuum model for the eigenmodes of the sample. The enhancement factor is defined as in the experiment, i.e. the ratio between the maximum peak intensity and the average of the generation peak intensity over the other seven detuning conditions. In the case of full optical decoupling, the generation (photoelastic) constant in the probe (pump) SL was taken as 0.
  • 16
    • 62549091850 scopus 로고    scopus 로고
    • As the pumand probe electric fields enter Eqs. (1) and (2) of Ref. in a quadratic form, the effects (i)-(iv) appear as independent terms in the computed spectra, that can be considered or not for computing theoretical enhancement factors.
    • As the pump and probe electric fields enter Eqs. (1) and (2) of Ref. in a quadratic form, the effects (i)-(iv) appear as independent terms in the computed spectra, that can be considered or not for computing theoretical enhancement factors.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.