2016
DOI: 10.1364/oe.24.012142
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Second harmonic generation at 399 nm resonant on the ^1S_0−^1P1 transition of ytterbium using a periodically poled LiNbO_3 waveguide

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Cited by 21 publications
(8 citation statements)
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References 50 publications
(34 reference statements)
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“…The case is important due to the strong electric dipole tran-sition between ground and excited 4f 14 6s6p 1 P o 1 state. It strongly dominates in the polarizability of Yb [49], it can be used in cooling [52], etc. The experimental value for the electric dipole amplitude is 4.148 a.u.…”
Section: Ytterbium Atommentioning
confidence: 99%
“…The case is important due to the strong electric dipole tran-sition between ground and excited 4f 14 6s6p 1 P o 1 state. It strongly dominates in the polarizability of Yb [49], it can be used in cooling [52], etc. The experimental value for the electric dipole amplitude is 4.148 a.u.…”
Section: Ytterbium Atommentioning
confidence: 99%
“…Frequency doubling was provided by a pig-tailed waveguide doubler and ~170 W output was obtained in the output fiber at 399 nm for ~50 mW in the fiber input at 798 nm. This doubler was supplied to us by AdvR [17] and is similar to that recently demonstrated by a group at the National Metrology Institute of Japan in collaboration with the NTT Electronics Corporation [18].…”
Section: Introductionmentioning
confidence: 99%
“…The full width at half maximum of this curve is 160 pm. As it is often reported elsewhere, experimental data deviate from the theoretical squared sine cardinal (sinc 2 ) shape and show a strong asymmetry [20,[25][26][27]. This results from inhomogeneity of the polling period or of the geometry or the index of the guide (thermal distribution, doping concentration inhomogeneity, etc.)…”
Section: Fig 2 Photograph Of the Sfg -Ppln Waveguide Modulementioning
confidence: 81%