1973
DOI: 10.1007/bf00939108
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Long-wave IR spectra of rare-earth metal oxysulfides

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Cited by 6 publications
(3 citation statements)
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“…[9] In the phonon calculations of R 2 O 2 S/R 2 O 3 , Raman-active modes are well reproduced, while IR-active modes are not, at the first glance. Unfortunately, only a few IR experimental works performed in 1970s are available [26,27]. We suspect the accuracy of the experimental data, as discussed in Ref.…”
Section: Resultsmentioning
confidence: 96%
“…[9] In the phonon calculations of R 2 O 2 S/R 2 O 3 , Raman-active modes are well reproduced, while IR-active modes are not, at the first glance. Unfortunately, only a few IR experimental works performed in 1970s are available [26,27]. We suspect the accuracy of the experimental data, as discussed in Ref.…”
Section: Resultsmentioning
confidence: 96%
“…It indicates that the amorphous phase of the precursor is converted to hexagonal Gd 2 O 2 S.The IR spectrum of the sulfurized sample (Fig.12a) displays essentially a peak at 447 cm À1 . The wavelength IR spectra of several rare earth oxysulfides have been investigated by Golovin et al,14 all the vibrational modes are below 500 cm À1 . The only band observed within the range of our apparatus is assigned to the Gd-O vibrations (E u type) and is actually composed of a main peak at 430 cm À1 and a shoulder at 475 cm À1 .…”
mentioning
confidence: 99%
“…These emissions are known to occur via classical energy transfer from Yb 3+ ions (sensitizers) to Tm 3+ ions (activators) and are quite specific of 3 H 4 → 3 H 6 , 3 F 3 → 3 H 6 , 1 G 4 → 3 F 4 and 1 G 4 → 3 H 6 transitions respectively. [16,25,26] The emission intensities are quite dependent on the proportion of doping elements. Consequently, we evaluated the impact of different proportions of Yb 3+ /Tm 3+ on the main emission peaks to primarily boost the NIR emission (802 nm) which is the most interesting for tissue penetration and bioimaging.…”
Section: Nps Characterizationmentioning
confidence: 99%