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84894397598
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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.
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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.
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0001458511
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84894392741
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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.
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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.
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84894389707
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