1994
DOI: 10.1007/3-540-58155-3_1
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Vibrational structure in the luminescence spectra of ions in solids

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Cited by 10 publications
(5 citation statements)
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“…24 In this dilute limit, the vibronic structure was attributed to a pseudo-secondorder Jahn−Teller distortion, where the Bi ions shifted away from the center of the regular octahedra to create one short and one long axial bond length. 25 These previous reports found several sharp emission lines on top of a broader band, much like in the spectra seen here for Cs 3 Bi 2 Br 9 , albeit only at liquidhelium temperatures.…”
supporting
confidence: 87%
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“…24 In this dilute limit, the vibronic structure was attributed to a pseudo-secondorder Jahn−Teller distortion, where the Bi ions shifted away from the center of the regular octahedra to create one short and one long axial bond length. 25 These previous reports found several sharp emission lines on top of a broader band, much like in the spectra seen here for Cs 3 Bi 2 Br 9 , albeit only at liquidhelium temperatures.…”
supporting
confidence: 87%
“…Similar luminescent properties have been reported when small concentrations of absorbing ions containing a pair of s 2 electrons (such as Bi 3+ , Sb 3+ , or Pb 2+ ) were substituted into nonabsorbing matrixes like Cs 2 NaYCl 6 . In this dilute limit, the vibronic structure was attributed to a pseudo-second-order Jahn–Teller distortion, where the Bi ions shifted away from the center of the regular octahedra to create one short and one long axial bond length . These previous reports found several sharp emission lines on top of a broader band, much like in the spectra seen here for Cs 3 Bi 2 Br 9 , albeit only at liquid-helium temperatures.…”
supporting
confidence: 76%
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“…As shown in the figure insets, of these crystals only CaMoO 4 shows noticeable emission at room temperature, the other two start to emit light at 30 (MgMoO 4 ) and 250 K (CdMoO 4 ). The emission spectra have composite structure and by analogy with the tungstate crystals the high-energy band is used to be interpreted as the radiative recombination of the electron-hole pairs localised at the MoO 4 2group [9]. The low-energy part of the spectrum is tentatively assigned to defect emission.…”
Section: Research Lettermentioning
confidence: 99%
“…However, in the present case, the emission band of the self‐luminescence of “WO 2 ” group is structureless. The large Stokes shift (~20 400 cm −1 ) in NWOF, arising from the extensive electronic redistribution between O 2− and W 6+ after charge transfer, should be responsible for the absence of vibrational structure . Moreover, the degeneracy of the electronic levels may be lifted in the highly distorted [WO 2 F 4 ] 2− octahedron, which also results in the disappearance of the fine structure in the PL spectrum, as proposed by Srivastava et al…”
Section: Resultsmentioning
confidence: 79%