We demonstrated passively Q-switched mode-locking in a laser-diode pumped c-cut Nd:GdVO 4 laser with a Cr 4ΓΎ :YAG crystal as the intracavity saturable absorber. At a pump power of 17.3 W, the Q-switched envelope repetition rate was 37 kHz with the maximum average output power of 2.1 W, while the mod
Q-switched mode-locking with Cr4+ : YAG in a diode pumped Nd : GdVO4laser
β Scribed by S. Zhang; E. Wu; H. Pan; H. Zeng
- Publisher
- Springer
- Year
- 2004
- Tongue
- English
- Weight
- 135 KB
- Volume
- 78
- Category
- Article
- ISSN
- 0721-7269
No coin nor oath required. For personal study only.
π SIMILAR VOLUMES
We demonstrate a diode-pumped passively Q-switched and mode-locking intracavity frequency-doubled Nd:GdVO~4~/KTP green laser with a Cr^4+^:YAG saturable absorber. Nearly 95% modulation depth for the mode-locked pulses inside the Q-switched envelope has been obtained. The Q-switched envelope pulses w
A passively Q-switched and mode-locked c-cut Nd:LuVO4 laser at 1.06 ΞΌm using Cr 4+ :YAG absorber has been successfully demonstrated. A nearly 100% modulation depth of mode-locking was achieved. At pump power of 12.04 W, the maximum average output power of 0.64 W and Q-switched pulse envelop repetiti
The realization of high repetition rate passively Q-switched monolithic microlaser is a challenge since a decade. To achieve this goal, we report here on the first passively Q-switched diode-pumped microchip laser based on the association of a Nd:GdVO 4 crystal and a Cr 4+ :YAG saturable absorber. T
A diode-pumped actively Q-switched and modelocked Nd:GdVO4 laser with great average output power and high efficiency was realized by using a comparative simple configuration and a short cavity length. The laser generates stable mode-locked pulses of estimated width 240 ps lying underneath a Q-switch
We report on the passively Q-switched mode-locking of a quasi-cw (QCW) diode pumped Nd:GdVO 4 laser with Cr 4+ :YAG saturable absorber. We show that by using the QCW pumping high quality Q-switched mode-locking can be easily obtained in the laser even with a simple two-mirror laser cavity configurat