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Cr4+ :YAG passive Q-switch
Cr4+ :YAG is an excellent passive Q-switch crystal for 0.8 to 1.2 µm lasers such as
Nd:YAG, Yb:YAG laser. Cr4+ :YAG is chemically stable, durable, UV resistant, good
thermal conductivity and high damage threshold. Cr4+ :YAG can also be used as
a laser crystal tuable at 1340 - 1580nm.
Advantages of Cr4+:YAG vs active acousto-optic and electro-optic Q-switch:
- No high voltage power supply needed
- Compact diffusion bonding available
- Higher reliability & longer lifetime
- Lower cost OEM components
Properties of Cr4+ :YAG Crystal
Chemical Formula: Cr4+ Y3 Al5 O12
Crystal Structure: Cubic Garnet
Lattice Constants: 12.01Å
Melting Point: 1970°C
Density: 4.56 g/cm³
Mohs Hardness: 8.5
Specific Heat: 0.59 J/g.cm³
Modulus of Elasticity: 310 Gpa
Young's Modulus: 3.17X104 Kg/mm2
Poisson Ratio: 0.3 (est.)
Tensile Strength: 0.13~0.26 GPa
Thermal Expansion Coefficient: 7.8 x 10-6 /K [111], 0-250°C
Thermal Conductivity: 12.13 W/m /K
Cr:YAG Optical Properties
Refractive Index: 1.82 @1064 nm
Lasing Wavelength: 1340 – 1580nm
Emission state absorption cross section: 8.2 x 10-19 cm²
Base state absorption cross section: 4.3 x 10-18 cm²
Flouresence Lifetime: 3.4 μs
Sellmeier equation( λ in μm):
n2 =2.08745+1.2081 λ2 /(λ2 -0.02119 )+17.2049 λ2 /(λ2 -1404.45)
General Specifications of Yb:YAG Laser Crystal
1) Orientation: <111>, <110>, <100> crystalline direction (+/-0.5°)
2) Wavefront Distortion: λ/8 per inch
3) Surface quality: 10/5 Scratch/Dig
4) Parallelism: 10 arc seconds
5) Perpendicularity: 5 arc minutes
6) Surface flatness: λ/10 at 633 nm
7) Clear aperture: Central 95%
8) Chamfer: 0.15mm @45°
9) Damage threshold: >1GW/cm² ns pulse
10) Dopant Level: 0.5 mol% ~ 3 mol%
i. Cr4+ :YAG crystal
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References:
1. Performance of a Cr: YAG laser
H. Eilers; W.M. Dennis; W.M. Yen; S. Kuck; K. Peterman; G. Huber
IEEE Journal of Quantum Electronics (Volume: 29, Issue: 9, September 1993)
Abstract:
We report on the performance of a Cr/sup 4+/:YAG laser, tunable over the range from 1.32 to 1.53 mu m, under different operating conditions. Laser action has been achieved by pumping with a Nd:YAG laser in the Q-switched mode and cw mode and with a Cr:Nd:GSGG laser in the long pulse mode. Slope efficiencies up to 22% in the Q-switched mode have been achieved. The lowest threshold was 30 mJ for the long pulse pumped mode. Excited state absorption seems to limit the tuning range and the output characteristics.
2. High peak power, passively Q-switched Yb: YAG/Cr: YAG micro-lasers
Masaki Tsunekane; Takunori Taira et al.
IEEE Journal of Quantum Electronics, Volume: 49 Issue: 5 May 2013
Abstract:
A high peak power (> MW), passively Q-switched Yb:YAG/Cr:YAG micro-laser end-pumped by fiber-coupled 120-W QCW LDs (Repetition rate 100 Hz) is developed. The convex output coupler with a curvature of -2 m successfully enlarges the fundamental mode size in the micro-laser cavity, and the output pulse energy increases to 3.6 mJ at a Cr:YAG initial transmission of 89% without optical damage. The TEM00 transverse mode and the single-frequency oscillation are confirmed. The pulse duration is 1.3 ns, and then the peak power is estimated as 2.8 MW. To our knowledge, these are the highest pulse energy and peak power ever reported in Yb:YAG/Cr:YAG micro-lasers. The Yb:YAG rod with 5 at.% Yb concentration and 4.2-mm thickness keeps more than 80% single-pass pump absorption ranging from 15°C to 45 °C in LD temperature. On the other hand, the characteristic temperatures of Yb:YAG/Cr:YAG and Nd:YAG/Cr:YAG lasers were estimated as 110 and 278 K, respectively. This means that the ratio of the increase in threshold pump energy to temperature of a Yb:YAG/Cr:YAG laser is twice or higher than that of a Nd:YAG/Cr:YAG laser due to a quasi-3-level system of Yb:YAG.
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