1964
DOI: 10.1080/00268976400100321
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Hypersensitive pseudoquadrupole transitions in lanthanides

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Cited by 874 publications
(230 citation statements)
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“…Jørgensen and Judd suggested that inhomogeneities in the dielectric surrounding the lanthanide ion could enhance the intensity of a hypersensitive transition [263]. According to this theoretical model, the electric field induces oscillating dipole moments in the ligands, which become secondary sources of radiation.…”
Section: Hypersensitivitymentioning
confidence: 99%
“…Jørgensen and Judd suggested that inhomogeneities in the dielectric surrounding the lanthanide ion could enhance the intensity of a hypersensitive transition [263]. According to this theoretical model, the electric field induces oscillating dipole moments in the ligands, which become secondary sources of radiation.…”
Section: Hypersensitivitymentioning
confidence: 99%
“…Such transitions are termed as hypersensitive transitions by Jorgensen and Judd [23]. These transitions are found to obey the selection rule ∆J≤2, ∆L≤2 and ∆S=0 [23].…”
Section: According To Judd-ofelt Theory [20 21] the Oscillator Strenmentioning
confidence: 99%
“…Such transitions are termed as hypersensitive transitions by Jorgensen and Judd [23]. These transitions are found to obey the selection rule ∆J≤2, ∆L≤2 and ∆S=0 [23]. These transitions are associated with a very large value of the reduced matrix element U 2 2 ; hence hypersensitivity is much related with the Ω 2 parameter.…”
Section: According To Judd-ofelt Theory [20 21] the Oscillator Strenmentioning
confidence: 99%
“…Since the upconversion emissions of Er 3+ ions are hypersensitive to the surroundings in comparison to Tm 3+ optical transitions ( Figure S2, Supporting Information). [ 23 ] Both the Er 3+ green and red upconversion emissions (including the line shape and position) are distinctively different in glassy and crystalline matrix ( Figure S2, Supporting Information). This spectroscopic feature is in particular useful to distinguish the Er 3+ ions in the nanocrystalline lattice from those diffused into the amorphous glass matrix, since the Er 3+ ions in the glassy environment show an absence of fi ne-structure spectroscopic features, which are observed for Er 3+ ions in the crystalline host.…”
Section: Resultsmentioning
confidence: 99%
“…[ 10b,34 ] By contrast, Er 3+ ions coordinated in crystalline sites in the NCs suspension give rise to upconversion spectra with a distinct fi ne structure. Although the Stark splitting of Er 3+ optical transitions occurs in both glass matrix and crystalline lattice, the Stark splitting of the continuum of different Er 3+ coordination sites in the glass matrix smears to broad bands, [ 23 ] whereas the similarity of Stark splitting of Er 3+ ions in crystalline sites results in narrow and distinct emissions. Consequently, the existence of the same fi ne-structure upconversion spectra between NCs-doped TZN glasses and LiYF 4 :Yb,Er NCs suspension demonstrates the survival of doped NCs in the TZN glass melt (Figure 3 a-c, and Figure S9, Supporting Information, different amounts of NCs in TZN glass).…”
Section: Full Paper Full Paper Full Papermentioning
confidence: 99%