Ce:LiCAF
Ce:LiCAF is perhaps the most extensively studied as a laser and amplifier material because of the absence of color center formation and solarization effects, therefore enabling high-power UV emission. Efficient UV generation through lasing techniques and/or amplification heavily relies on crystal quality and pumping configuration. The gain spectra of Ce:LiCAF is in the range 280–320 nm and is characteristic of the Ce3+ 5d1–4f1 interconfigurational transition. Ce3+-doped colquiriite LiCaA1F6 single crystals (LiCAF:Ce) are not only excellent u.v. fluorescers, but they also exhibit broadband tunable gain in u.v. under pulsed pumping at 266nm. UV solid-state laser materials that are continuously tunable over 4000cm−1, such as and Ce:LiCAF, could service numerous scientific, engineering, and medical applications. This material may also be suited to remote-sensing applications, since molecules such as ozone and aromatic-based compounds have characteristic absorption bands in the UV. For example, the UV tunability provided by Ce:LiCAF could serve as the basis for a UV differential-absorption lidar system that would have the versatility of continuously variable wavelengths. The reliability, compactness, nontoxicity, and high efficiencies offered by solid-state lasers provide many advantages over other tunable coherent ultraviolet sources, such as frequency-doubled dye lasers. Applications in inhospitable environments may also be rendered more practical with an all-solid-state UV source.
Parameter
Orientation Tolerance | 5ˊ |
Parallelism | <10〞 |
Perpendicularity | 5ˊ |
Chamfer | 0.1mm@45° |
Surface Quality | 10/5 or better |
Wavefront Distortion | λ/8 @632.8 nm |
Surface Flatness | λ/10 @632.8 nm |
Clear Aperture | >95% |
Diameter Tolerance | +0/-0.05mm |
Length Tolerance | ±0.1mm |
Coatings | As per requirement |
Dopant Concentration Tolerance | 0.10% |
Crystal Structure | Trigonal |
Space Group | P31C |
Lattice Constants | a=4.9808, c=9.6052Å@1mol%CeF3 |
Density (g/cm3) | 2.94 |
Melting Point | 766°C |
Thermal Conductivity(W·m-1·K-1) | 3.09-2.9 |
Thermal Expansion(10-6K-1) | 24.3(∥a), 2.7(∥c) |
Absorption Peak Wavelength(nm) | 640 |
Absorption Cross-section(10-18cm2)@266nm | 7.3(π), 5.8(σ) |
Absorption Coefficient@266nm | 4cm-1 |
Refractive Index | n=1.41 |
Laser Wavelength(nm) | 266 |
Fluorescence Lifetime(μs) | 25 |
Spontaneous Emission Constant(10-10cm·s-2) | 0.2 |
Emission Cross-section(10-18cm2)@290nm | 9.6(π), 6.2(σ) |
Laser Threshold(μJ) | 15-25 |
Estimated Pumping Efficiency | 50(π), 33(σ) |
ESA Cross-section(10-18cm2)@266nm | 5.5π), 6.2(σ) |
Gain Cross-section(10-18cm2)@290nm | 6.0(π), 4.0(σ) |
Saturation Fluence(mJ/cm2) | 115 |
- The gain spectra of Ce:LiCAF are in the range 280–320 nm
- Characteristic of the Ce3+5d1–4f1 interconfigurational transition
- Absence of solarization effects
- Transparency, tolerance to laser-induced damage
- o be directly pumped
- Can be directly pumped at 266 nm by the fourth harmonic generation of Nd:YAG laser
- Broad UVtunability (from 280 to 325 nm)
- Scintillator
- Tunable ultraviolet lasers
- Remote-sending applications
- Ultrafast pulse generation and amplification
- Power UV laser amplifiers
[1] Maria, Luisa, Grilli, et al. Al2O3/SiO2 and HfO2/SiO2 dichroic mirrors for UV solid-state lasers[J]. Thin Solid Films, 2009. |
[2] Bayramian A J , Marshall C D , Wu J H , et al. Ce:LiSrAlF6 Laser Performance with Antisolarant Pump Beam[J]. Journal of Luminescence, 1996, 69(2):85-94. |
[3] Yamaji A , Yokota Y , Yanagida T , et al. Crystal growth and dopant segregation of Ce:LiSrAlF_6 and Eu:LiSrAlF_6 crystals with high dopant concentrations[J]. Journal of Crystal Growth, 2012, 352(1):p.106-109. |
[4] Mcgonigle A , Coutts D W , Girard S , et al. A 10 kHz Ce:LiSAF laser pumped by the sum-frequency-mixed output of a copper vapour laser[J]. Optics Communications, 2003, 193(1-6):233-236. |
[5] Tanaka C , Yokota Y , Kurosawa S , et al. Crystal growth and optical properties of indium doped LiCaAlF6 scintillator single crystals[J]. Optical Materials, 2016:S092534671630595X. |
[6] Yamaji A , Yanagida T , Kawaguchi N , et al. Crystal growth and scintillation properties of Ce and Eu doped LiSrAlF_6[J]. Nuclear Instruments & Methods in Physics Research, 2011, 659(1):p.368-372. |
[7] Watanabe K , Yamazaki T , Dai S , et al. Wavelength-shifting fiber signal readout from Transparent RUbber SheeT (TRUST) type LiCaAlF6 neutron scintillator[J]. Nuclear Inst & Methods in Physics Research A, 2015, 784(jun.1):260-263. |
[8] Yanagida T , Fujimoto Y , Yamaji A , et al. Study of the correlation of scintillation decay and emission wavelength[J]. Radiation Measurements, 2013, 55:99-102. |
[9] Shavelev A A , Nizamutdinov A S , Marisov M A , et al. Single crystals with advanced laser properties LiCaAlF 6 :Ce 3+ grown by Bridgman technique[J]. Journal of Crystal Growth, 2018, 485:73-77. |
[10] Neutron–gamma discrimination based on pulse shape discrimination in a Ce:LiCaAlF 6 scintillator[J]. Nuclear Instruments & Methods in Physics Research, 2011, 652(1):435-438. |
[11] Castillo V K , Quarles G J . Progress in the crystal growth of Ce : colquiriites[J]. Journal of Crystal Growth, 1997, 174(1):337–341. |
[12] Spectroscopic properties of UV active medium Ce3+:LiSr0.8Ca0.2AlF6[J]. Optical Materials, 2016, 52:157-162. |
[13] Spence D J , Liu H , Coutts D W . Low-threshold miniature Ce:LiCAF lasers[J]. Optics Communications, 2006, 262(2):238-240. |
[14] K Shimamura and H Sato and A Bensalah and H Machida and N Sarukura and T Fukuda. Growth of Ce-doped Colquiriite- and Scheelite-type single crystals for UV laser applications[J]. Optical Materials, 2002. |
[15] Tsuboi T , Petrov V , Noack F , et al. Femtosecond relaxation in Ce3+ ions in LiCaAlF6 and LiSrAlF6[J]. Journal of Alloys & Compounds, 2001, 323(none):688-691. |
[16] A M A F , A B E O , A M C , et al. Evaluation of Eu:LiCAF for neutron detection utilizing SiPMs and portable electronics[J]. Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 2018, 908:110-116. |
[17] Tanaka C , Yokota Y , Kurosawa S , et al. Growth and radioluminescence of metal elements doped LiCaAlF6 single crystals for neutron scintillator[J]. Radiation Measurements, 2016:170-173. |
[18] Liu Z , Shimamura K , Fukuda T , et al. High-energy pulse generation from solid-state ultraviolet lasers using large Ce:fluoride crystals[J]. Optical Materials, 2002, 19(1):123-128. |
[19] Micro-pulling-down-method-grown Ce:LiCAF crystal for side-pumped laser amplifier[J]. Journal of Crystal Growth, 2011, 318(1):737-740. |
[20] Shiran N , Gektin A , Neicheva S , et al. Energy storage in Ce-doped LiCaAlF 6 and LiSrAlF 6 crystals[J]. Radiation Measurements, 2004, 38(4-6):459-462. |
[21] Tanaka C , Yokota Y , Kurosawa S , et al. Effects of Na co-doping on optical and scintillation properties of Eu:LiCaAlF6 scintillator single crystals[J]. Journal of Crystal Growth, 2016:S0022024816306984. |
[22] Yokota Y , Tanaka C , Kurosawa S , et al. Effects of Ca/Sr Ratio Control on Optical and Scintillation Properties of Eu-doped Li(Ca,Sr)AlF 6 Single Crystals[J]. Journal of Crystal Growth, 2018, 490:71-76. |
[23] Johnson K S , Pask H M , Withford M J , et al. Efficient all-solid-state Ce:LiLuF laser source at 309 nm[J]. Optics Communications, 2005, 252(1):132-137. |
[24] Yanagida, T, Yoshikawa, et al. Crystal growth, optical properties, and a-ray responses of Ce-doped LiCaAlF6 for different Ce concentration[J]. OPTICAL MATERIALS -AMSTERDAM-, 2009. |
[25] Yoshikawa A , Iguchi T , Boulon G , et al. Development of novel rare earth doped fluoride and oxide scintillators for two-dimensional imaging[J]. Journal of Rare Earths, 2011, 29(012):1178-1182. |
[26] Iwanowska J , Swiderski L , Moszynski M , et al. Thermal neutron detection with Ce 3+ doped LiCaAlF 6 single crystals[J]. Nuclear Instruments & Methods in Physics Research, 2011, 652(1):319-322. |
[27] None. Author index to volumes 251–260[J]. 1996, 251-260(index-I):1-79. |
[28] Shiran N , Gektin A , Neicheva S , et al. Energy transfer in pure and Ce-doped LiCaAlF6 and LiSrAlF6 crystals[J]. Nuclear Inst & Methods in Physics Research A, 2005, 537(1/2):266-270. |
[29] Fedyanin D Y , Arsenin A V . Stored light in a plasmonic nanocavity based on extremely-small-energy-velocity modes[J]. Photonics and Nanostructures – Fundamentals and Applications, 2010, 8(4):264-272. |
[30] Uesaka M , Tagi K , Dobashi K , et al. 30 MeV X-band Electron Linac Neutron Source for Nuclear Data Study for Fukushima Accident Analysis[J]. Physics Procedia, 2014, 60:193-202. |
Leave a Reply