1989
DOI: 10.1016/0022-2313(89)90052-5
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Optical spectroscopy of the new laser materials, LiSrAlF6:Cr3+ and LiCaAlF6:Cr3+

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Cited by 124 publications
(67 citation statements)
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“…The presence of octahedral sites is due to strong ligand field stabilization energy of Cr 3+ ions in six-fold coordination. The parity-forbidden d-d transitions may be due to partially allowed by weak distortion of the crystal field or by instantaneous distortion due to molecular vibrations [30][31][32][33][34]. Here, the E opt values are 3.43eV, 2.71eV, 3.39eV and 3.36eV for LPZ glass, NPZ glass, KPZ glass and PZ glass [23] respectively.…”
Section: Resultsmentioning
confidence: 93%
“…The presence of octahedral sites is due to strong ligand field stabilization energy of Cr 3+ ions in six-fold coordination. The parity-forbidden d-d transitions may be due to partially allowed by weak distortion of the crystal field or by instantaneous distortion due to molecular vibrations [30][31][32][33][34]. Here, the E opt values are 3.43eV, 2.71eV, 3.39eV and 3.36eV for LPZ glass, NPZ glass, KPZ glass and PZ glass [23] respectively.…”
Section: Resultsmentioning
confidence: 93%
“…The absorption oscillator strength f abs was evaluated from the absorption spectrum by the relation [13] f abs 9n…”
Section: Emission Spectra Analysismentioning
confidence: 99%
“…Since the impurity is nearly always situated in octahedral sites, the absorption and emission spectra are similar in a large variety of materials, the main distinction being the strength of the octahedral field, rather than its exact nature (59) This is well demonstrated by the absorption and emission spectra of ruby, alexandrite, and Cr:Li-SAF, the materials illustrated in this section. The absorption spectra at lower energies are all characterized by two broad bands corresponding to the transitions, with the positions of the peaks changing according to the field strength.…”
Section: Methodsmentioning
confidence: 83%