Cr,Tm,Ho:YAG

Cr,Tm,Ho:YAG

Cr, Tm, Ho: YAG is a high efficient laser crystal pumped by a Xenon lamp or diode with a wavelength of 2.1μm. The pump source mainly originates from the flashlamp energy absorbed by Cr3+, Ho3+ is a working ion, and Tm3+ acts as an intermediary to transfer energy. 2.1 μm laser wave can be absorbed by water very well, transmits atmosphere easily, and is safe to the eye. Therefore, it is widely used in medical treatment, laser radar, the military, etc. Moreover, a 2.1 μm laser is an ideal pump source for a 3-5 μm mid-infrared optical parametric oscillator.

Cr, Tm, Ho: YAG is a highly efficient laser crystal pumped by a Xenon lamp or diode with a wavelength of 2.1μm. The pump source mainly originates from the flashlamp energy absorbed by Cr3+. Ho3+ is a working ion, and Tm3+ acts as an intermediary to transfer energy. 2.1 μm laser wave can be absorbed by water very well, transmits atmosphere easily, and is safe to the eye. Therefore, it is widely used in medical treatment, laser radar, the military, etc. Moreover, a 2.1 μm laser is an ideal pump source for a 3-5 μm mid-infrared optical parametric oscillator.

  • Wide absorption band
  • Working at room temperature
  • 2.1 mm lasing wavelength is for the eye
  • High slope efficiency
  • It can be pumped by a flashlamp or diode

Material Specifications

Doping ConcentrationHo:0.3~0.4at% Cr:0.3~1.2at% Tm:5~6at%
Wavefront Aberration<λ/4@632nm
Extinction Ratio≥25 dB
SizeDiameter:3~6mm,Length:50~120mm
Size ToleranceDiameter:+0.00/-0.05mm, Length: ± 0.5mm
Precision Grinding50-80 Micro Inches(RMS)
Parallelism≤30″
Perpendicularity≤5′
Flatnessλ/10@ 633 nm
Surface Finish10/5 Scratch / Digper MIL-O-1380A
Chamfer0.006″±0.002″ at 45°± 5°
High Permeable Film Reflectivity≤ 0.25% (@2094nm)

Physical and Chemical Properties

StructureCubic
Lattice Constant12.01Å
Melting Point1970°C
Density4.56g/cm3
Orientation<111> or <100]> 5°
Thermal Expansion7.8×10-6 /K
Coefficient of Thermal Conductivity14W/m/K, 20°C;10.5W/m/K, 100°C
Mohs hardness8.5
Dielectric Constant11.7

Optical and Spectral Properties

Laser Transition5I7 → 5I8
Laser Wavelength 2.094 µm
Photon Energy9.55 x 10–20 J
Radiation Cross Section7 x 10-21 cm2
Fluorescence Lifetime 8.5 ms
Refractive Index1.80 @2.08 µm
Aperture>90%
Absorption Line Width4 nm
Diode Pump Band781 nm
Main Pump Belt400~800 nm

Absorption and Emission Spectra

CrTmHo-YAG-laser-crystal-emission-spectrum-CRYLINKCrTmHo-YAG-laser-crystal-absorption-spectrum-CRYLINK

References

[1]  Tonelli M ,  Falconieri M ,  Lanzi A , et al. Comparison of Tm-sensitized Ho:Yag and Ho:YLF crystals for a laser-pumped 2 μm CW oscillator[J]. Optics Communications, 1996, 129(1-2):62-68.
[2]  Kaczmarek S M ,  ?Endzian W ,  ?Ukasiewicz T , et al. Effects of gamma irradiation and annealing treatments on the performance of Cr;Tm;Ho:YAG lasers[J]. Spectrochimica Acta Part A Molecular and Biomolecular Spectroscopy, 1998, 54(13):2109-2116.
[3]  Cheng L ,  Shen D ,  Jie S , et al. Flash-lamp pumped normal-mode and Q-switched Cr–Tm:YAG laser performance at room temperature[J]. Optics Communications, 1999, 164(1-3):63-67.
[4] M, Falconieri, and, et al. Fluorescence dynamics in an optically-excited Tm,Ho:YAG crystal[J]. Optical Materials, 1997.
[5]  Zhang H ,  Sun D ,  Luo J , et al. Growth and spectroscopic properties of the 2.9μm Tm,Ho:LuYAG laser crystals[J]. Optical Materials, 2015, 47:490-494.
[6]  Dou R ,  Zhang Q ,  Liu W , et al. Growth, structure, chemical etching, and spectroscopic properties of a 2.9 μm Tm,Ho:GdYTaO4 laser crystal[J]. Optical Materials, 2015, 48:80-85.
[7]  Yang X T ,  Mu Y L ,  Zhao N B . Ho:SSO solid-state saturable-absorber Q switch for pulsed Ho:YAG laser resonantly pumped by a Tm:YLF laser[J]. Optics & Laser Technology, 2018, 107:398-401.
[8] R Müller,  Fuhrberg P ,  Teichmann H O , et al. Pulsed and cw Cr,Tm:YAG laser with simultaneous diode and flashlamp excitation[J]. Optics & Laser Technology, 2005, 37(7):570-576.
[9] Liu, C, Zhao, et al. Stable kilo-hertz electro-optically Q-switched Tm,Ho:YAP laser at room temperature.[J]. Optics & Laser Technology, 2016.
[10]  Lancaster D G ,  Dawes J M . Thermal-lens measurement of a quasi steady-state repetitively flashlamp-pumped Cr, Tm, Ho:YAG laser[J]. Optics & Laser Technology, 1998, 30(2):103-108.
[11]  Saiki T ,  Motokoshi S ,  Imasaki K , et al. Two-pass amplification of CW laser by Nd/Cr:YAG ceramic Active mirror under lamp light pumping[J]. Optics Communications, 2009, 282(5):936-939.

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