2017
DOI: 10.1016/j.optmat.2016.09.062
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First-principles calculations of electronic and optical properties of LiCaAlF 6 and LiSrAlF 6 crystals as VUV to UV solid-state laser materials

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Cited by 20 publications
(8 citation statements)
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“…If the conduction band minimum of the host is close to the 5d excited state level of the activator ion, then ESA will be greater in this laser material. Similar band structure and DOS calculations performed for LiSAF reveal that the band gap energy of LiSAF is 11.79 eV, which is 0.44 eV smaller than LiCAF [62]. Associated with the strong ESA is color center formation or solarization, which happens due to an electron getting trapped at impurities in the conduction band of the host as shown in Figure 6 [27].…”
Section: Numerical Simulation Of the Electronic Properties Of The Licmentioning
confidence: 59%
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“…If the conduction band minimum of the host is close to the 5d excited state level of the activator ion, then ESA will be greater in this laser material. Similar band structure and DOS calculations performed for LiSAF reveal that the band gap energy of LiSAF is 11.79 eV, which is 0.44 eV smaller than LiCAF [62]. Associated with the strong ESA is color center formation or solarization, which happens due to an electron getting trapped at impurities in the conduction band of the host as shown in Figure 6 [27].…”
Section: Numerical Simulation Of the Electronic Properties Of The Licmentioning
confidence: 59%
“…Ultrashort Pulse Generation in Ce:LiCAF Ultraviolet Laser http://dx.doi.org/10.5772/intechopen.73501 energies of the LiCAF crystal. These calculations employed the projector-augmented wave (PAW) method as implemented within the Vienna Ab Initio Simulation Package (VASP) [52][53][54][55][56][57], with a plane-wave basis cutoff of 500 eV and a hybrid density functional, which uses the full Perdew-Burke-Ernzerhof (PBE) [58,59] correlation energy but mixes 65% PBE exchange with 35% exact exchange [60][61][62][63]. The initial charge density and wave function was generated using a 3 Â 3 Â 1 Monkhorst-Pack k-point grid.…”
Section: Numerical Simulation Of the Electronic Properties Of The Licmentioning
confidence: 99%
“…The respective spectra of the input pulses are depicted by dashed curves. λ p = 1030 nm λ p = 800 nm λ p = 400 nm λ p = 515 nm crystal, which has very similar optical characteristics as LiSAF, and exhibits a slightly larger energy bandgap (12.23 eV [25]) and somewhat better transparency in the UV, with a short-wavelength absorption edge at 112 nm [26]. Figure 4 presents the SC spectra generated in the 5 mm-long LiCAF sample (Optogama) using the pump beams with parameters listed in Table 1.…”
Section: Resultsmentioning
confidence: 99%
“…The latter application indirectly suggests that the LiSAF crystal itself is highly resistable to intense UV irradiation. In addition to that, LiSAF exhibits an excellent set of optical properties: a very large energy bandgap of 11.79 eV [25], a shortwavelength absorption edge at 116 nm [26], a low refractive index and so a low chromatic dispersion throughout the UV, visible and near IR, that qualify this crystal as a potentially attractive material for SC generation.…”
Section: Introductionmentioning
confidence: 99%
“…Ce:LiCAF also has a large saturation fluence and damage threshold, making it attractive for designing power amplifiers [13,14]. Most importantly, color center formation or solarization was not observed from Ce:LiCAF, giving it the edge over Ce:LiSAF, which exhibits a lower laser efficiency due to excited state absorption and color center formation [12,15,16].…”
Section: Introductionmentioning
confidence: 99%