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Volumn 24, Issue 5, 2007, Pages 1037-1041

Generation of a continuous-wave pulse train at a repetition rate of 17.6 THz

Author keywords

[No Author keywords available]

Indexed keywords

CONTINUOUS WAVE LASERS; DISPERSION (WAVES); LASER RESONATORS; LIGHT EMISSION; STIMULATED RAMAN SCATTERING;

EID: 34250703237     PISSN: 07403224     EISSN: None     Source Type: Journal    
DOI: 10.1364/JOSAB.24.001037     Document Type: Article
Times cited : (23)

References (22)
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    • The longitudinal modes contributing to the generation of the Stokes emissions differed between the spectrum shown in Fig. 2(a) and that shown in Fig. 3(b). Owing to the bandwidth of a Raman gain, the efficiency for both Stokes emissions varied depending on the related longitudinal modes even when the pump power was constant.
    • The longitudinal modes contributing to the generation of the Stokes emissions differed between the spectrum shown in Fig. 2(a) and that shown in Fig. 3(b). Owing to the bandwidth of a Raman gain, the efficiency for both Stokes emissions varied depending on the related longitudinal modes even when the pump power was constant.
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    • s1-s2. At the wavelength of P (770.0 nm), n = 1.000137506, and dn /dλ = -4.67008. At the wavelength of S1 (806.5 nm), n = 1.000137345, and dn/dλ=-4.04611. At the wavelength of S2 (846.5 nm), n = 1.000137198 and dn/dλ = -3.50354.
    • s1-s2. At the wavelength of P (770.0 nm), n = 1.000137506, and dn /dλ = -4.67008. At the wavelength of S1 (806.5 nm), n = 1.000137345, and dn/dλ=-4.04611. At the wavelength of S2 (846.5 nm), n = 1.000137198 and dn/dλ = -3.50354.
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    • 3.
    • 3.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.