Pr:YLF
Pr3+:YLF has been found as promising laser material for producing visible lasers directly. Many trivalent rare-earth ions (RE3) exhibit visible radiative transitions that potentially enable visibly emitting solid-state lasers. So far, various visible lasers based on RE3+-doped crystalline media have been demonstrated. Among them, trivalent praseodymium ion (Pr3) is recognized as one of the most successful active ions for achieving efficient visible lasers because the visible transitions of Pr3+ follow a four-level system, and their emission cross sections are larger than that of other RE3+. Many other RE3+ also exhibit visible transitions; however, these are often spin-forbidden, resulting in very small absorption and emission cross sections. Moreover, some visible transitions in RE3+ follow a three-level system, which is unattractive for laser demonstration. Only few laser materials have necessary properties for realization of lasing in visible spectral range. Trivalent praseodymium (Pr3+) is known to be an interesting laser ion for using with solid-state lasers in the visible spectral range because of its energy levels scheme, providing several transitions in the red (640 nm, 3P0 to 3F2), orange (607 nm, 3P0 to 3H6), green (523 nm, 3P0 to 3H5), and dark-red (720 nm, 3P0 3F3+3F4) spectral regions.
Parameter
Orientation | a-cut |
Parallelism | <10〞 |
Perpendicularity | <10ˊ |
Surface Quality | 10-5 S-D |
Wavefront Distortion | <λ/4 per inch@632.8 nm |
Surface Flatness | <λ/8 @632.8 nm |
Clear Aperture | >90% |
Face Dimensions Tolerance | +0/-0.1 mm |
Length Tolerance | ±0.1mm |
Chamfer | 0.1mm@45° |
Coatings | R<1%@440-444nm+R<0.6%@500-700nm on both faces |
Laser Induced Damage Threshold | >5J/cm2@532nm, 10ns |
Structure Symmetry | Tetragonal |
Lattice Constants | a=5.164, c=10.732 Å |
Specific mass | 3.95g/cm3 |
Melting Point | 819°C |
Thermal Conductivity /(W·m-1·K-1) | 6 |
Thermal Expansion /(10-6·K-1 ) | ~16 |
Hardness ( @Mohs) | 5 |
Typical Doping Level | 1@.% |
Refractive Index (@1064nm) | no=1.448, ne=1.470 |
Thermo-optic Coefficient(10-6·K-1) | -5.2(∥c), -7.6(∥a) |
Lifetime of 3P0 Erbium Energy Level(μs) | 50 |
Emission Cross-section(10-20/cm2) | 20×10-20cm2 |
Absorption Peak Wavelength | 444nm |
Absorption Cross-section at Peak | 8×10-20cm2 |
Absorption Bandwidth at Peak Wavelength | ~5nm |
Laser Wavelength | 640nm |
- High absorption and emission cross-sections(~10-19cm2)
- Good overlapping of the absorption band in the blue spectral region withthe emission
- Lines of the InGaN laser diodes and 2ω-OPSL
- Custom crystals available upon request
- Diode-pumped solid-state lasers for precise and efficient processing of metals such as copper or gold, entertainment industry and science
- Broadband laser mirrors
- Wavelength separators and combiners
- Polarizing cubes
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[27] Few-layer Bi 2 Se 3 -based passively Q-switched Pr:YLF visible lasers |
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