2008
DOI: 10.1364/oe.16.018875
|View full text |Cite
|
Sign up to set email alerts
|

Kerr-lens mode-locked Ti:sapphire laser with an additional intracavity nonlinear medium

Abstract: We demonstrate a Kerr-lens mode-locked Ti:sapphire laser with an additional Yb(3+) doped Potassium Yttrium Tungstate crystal (Yb:KYW) in the laser cavity, where not only the pump threshold to start mode-locking but also the stable regions to maintain mode-locking can be well-controlled by varying the position of Yb:KYW nearby the confocal focus to change the intracavity Kerr-effects. The pump threshold is reduced down to 800 mW to start the mode-locking operation, which is about 27% less than that for a Ti:sap… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1

Citation Types

0
4
0

Year Published

2010
2010
2021
2021

Publication Types

Select...
4
2

Relationship

0
6

Authors

Journals

citations
Cited by 7 publications
(4 citation statements)
references
References 14 publications
0
4
0
Order By: Relevance
“…x,y 10) combined with large pump spot diameters in the laser crystal [294]. However, note that the additional telescope increases the range of paramters that need to be adjusted for modelocked operation, and changing the distances within one telescope critically affects the beam diameters in the other telescope [295]. A first step into this direction was also performed with the setup of MIRanda3 : by replacing the end-mirror (EM) in figure 5.6 with a spherical mirror (CM) (see figure 5.20), the short arm of the cavity was extended by an additional telescope.…”
Section: )mentioning
confidence: 99%
“…x,y 10) combined with large pump spot diameters in the laser crystal [294]. However, note that the additional telescope increases the range of paramters that need to be adjusted for modelocked operation, and changing the distances within one telescope critically affects the beam diameters in the other telescope [295]. A first step into this direction was also performed with the setup of MIRanda3 : by replacing the end-mirror (EM) in figure 5.6 with a spherical mirror (CM) (see figure 5.20), the short arm of the cavity was extended by an additional telescope.…”
Section: )mentioning
confidence: 99%
“…It can be especially beneficial for the laser systems where an MM LD is used for pumping. The use of an additional Kerr medium has been investigated for bulk KLM lasers [19,[21][22][23][24][25][26][27][28][29][30][31]. Recently, high power KLM lasers with MM LD pumping and an enhanced Kerr effect have been reported for Yb:Lu 2 O 3 ceramic (135 fs, 1.83 W) [21] and Yb:CALYO lasers (68 fs, 1.5 W) [19].…”
Section: Introductionmentioning
confidence: 99%
“…Intracavity second harmonic generation (SHG) in longitudinal diode end pumped Nd : YVO 4 lasers with KTP and LBO nonlinear crystals is a common method to produce continuous wave green lasers with low intensity noise and good beam quality. These systems have numerous applications in science and technology [1][2][3]. The main challenge in this type of laser is intensity noise due to nonlinear coupling of longitudinal modes, referred to as the green problem.…”
Section: Introductionmentioning
confidence: 99%