2012
DOI: 10.1016/j.jlumin.2011.10.012
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Temperature measurements inside an Er3+–Yb3+ co-doped fluoride crystal heated by a NIR laser diode and probed by red-to-green upconversion

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Cited by 16 publications
(4 citation statements)
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“…As predicted by the Boltzmann law, we find [13] that the logarithmic values of intensities ratio vary in a linear way with the inverse of temperature (Fig. 5).…”
Section: Temperature Measurement By Photoluminescence Of Doped Microcsupporting
confidence: 74%
“…As predicted by the Boltzmann law, we find [13] that the logarithmic values of intensities ratio vary in a linear way with the inverse of temperature (Fig. 5).…”
Section: Temperature Measurement By Photoluminescence Of Doped Microcsupporting
confidence: 74%
“…For example, a NIR laser can be employed as both excitation and heating source to heat up the UCL material. A thermocouple is in contact with the material to monitor the temperature 205,206 while some groups used furnace 23,207 or cooling-heating systems to precisely measure temperatures. [208][209][210] Vetrone et al built a set-up by using a pump-probe and a fibercoupled confocal microscope connected to a high-resolution spectrometer.…”
Section: Characterization Of Stimulus Responsementioning
confidence: 99%
“…As demonstrated above, NPs during the annealing process can be divided into amorphous, phase evolution, and the pure YAG state. The key UCLs centered at 556 and 546 nm are ascribed to stark splitting of 4 S 3/2 . As shown in Figure S7, the 4 S 3/2 stark splitting produces the high and low substark levels as 4 S 3/2(1) and 4 S 3/2(2) , emitting 556 and 546 nm UCLs through 4 S 3/2(1) → 4 I 15/2 and 4 S 3/2(2) → 4 I 15/2 processes, respectively. Figure b records the UCL intensity ratios of 556 and 546 nm, which are used as a characteristic parameter to evaluate the phase evolution state of NPs in the annealing process.…”
Section: Resultsmentioning
confidence: 97%