𝔖 Bobbio Scriptorium
✦   LIBER   ✦

Diode-end-pumped composite Nd:YVO4 yellow laser based on intracavity frequency-doubled self-Raman laser

✍ Scribed by Li Zhang; Yongqin Yu; Yayin Guo; Chenlin Du; Shuangchen Ruan


Publisher
Elsevier Science
Year
2010
Tongue
English
Weight
691 KB
Volume
283
Category
Article
ISSN
0030-4018

No coin nor oath required. For personal study only.


πŸ“œ SIMILAR VOLUMES


Diode-pumped Nd:LuVO4 and Nd:YAG crystal
✍ Y.F. LΓΌ; X.H. Zhang; X.H. Fu; J. Xia; T.J. Zheng; J.F. Chen πŸ“‚ Article πŸ“… 2010 πŸ› John Wiley and Sons 🌐 English βš– 77 KB

We present for the first time laser architecture to obtain continuous-wave yellow radiation at 594 nm. The choice of crystals (Nd:LuVO 4 for emission at 1343 nm and Nd:YAG for emission at 1064 nm) was guided by laser performance. A part of the pump power was then absorbed by the Nd:LuVO4 crystal, th

Efficient CW laser at 559 nm by intracav
✍ Y.F. LΓΌ; W.B. Cheng; Z. Xiong; J. Lu; L.J. Xu; G.C. Sun; Z.M. Zhao πŸ“‚ Article πŸ“… 2010 πŸ› John Wiley and Sons 🌐 English βš– 130 KB

We report an efficient continuous wave (CW) laser emission at 559 nm by sum-frequency mixing of the fundamental and first-Stokes fields generated within an Nd:YVO 4 self-Raman laser. Intracavity sum-frequency mixing with LiB 3 O 5 (LBO) nonlinear crystal yielded 890 mW of visible yellowgreen emissio

Continuous-wave yellow light source at 5
✍ Y.K. Bu; C.Q. Tan; N. Chen πŸ“‚ Article πŸ“… 2011 πŸ› John Wiley and Sons 🌐 English βš– 89 KB

We present a simple laser architecture to obtain continuous-wave (CW) true yellow light sources at the 579 nm. A 806 nm diode-pumped a Nd:YLF crystal emitting at 1047 nm with intracavity Raman shifting by SrWO 4 crystal at 1158 nm. Intracavity frequency-doubling at 1158 nm was then realized in a LiB

Theoretical and experimental study of a
✍ Kejian Yang; Shengzhi Zhao; Guiqiu Li; Hongming Zhao πŸ“‚ Article πŸ“… 2005 πŸ› Elsevier Science 🌐 English βš– 316 KB

By considering the Guassian spatial distribution of the intracavity photon density and the longitudinal distribution of the photon density along the cavity axis as well as the influence of turnoff time of the acoustic-optic Q-switch, the coupled rate equations of actively Q-switched intracavity freq