2019
DOI: 10.1016/j.jallcom.2019.01.087
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Enhanced photoluminescence and ultrahigh temperature sensitivity from NaF flux assisted CaTiO3: Pr3+ red emitting phosphor

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Cited by 56 publications
(7 citation statements)
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“…However, the emission intensity of 1 D 2 – 3 H 4 (612 nm) was constant and the emission peak broadened with the increase in temperature, resulting in a blue shift and broadening in the range of 580–630 nm. Similar experimental phenomena also appeared in previous research. ,,,, As the temperature rises, the electrons in the 3 P 0 state relax to the 1 D 2 state by Pr 3+ –Ti 4+ IVCT, resulting in the changing of the relative population between 3 P 0 and 1 D 2 states. Consequently, the FIR between 3 P 0 and 1 D 2 transitions can be strongly controlled with temperature.…”
Section: Results and Discussionsupporting
confidence: 84%
“…However, the emission intensity of 1 D 2 – 3 H 4 (612 nm) was constant and the emission peak broadened with the increase in temperature, resulting in a blue shift and broadening in the range of 580–630 nm. Similar experimental phenomena also appeared in previous research. ,,,, As the temperature rises, the electrons in the 3 P 0 state relax to the 1 D 2 state by Pr 3+ –Ti 4+ IVCT, resulting in the changing of the relative population between 3 P 0 and 1 D 2 states. Consequently, the FIR between 3 P 0 and 1 D 2 transitions can be strongly controlled with temperature.…”
Section: Results and Discussionsupporting
confidence: 84%
“…Thus, an important goal for Pr 3+ -doped oxide materials is to control the 3 P 0 → l D 2 radiationless transition and hence the relative intensities of the greenish-blue ( 3 P 0 → 3 H 4 ) and red ( 1 D 2 → 3 H 4 ) emissions via the IVCT state. Furthermore, the IVCT state of lanthanide-doped luminescence materials exhibits a great interest for not only fundamental studies but also technological applications, , particularly for optical temperature sensing Up to now, the most typical technique previously reported for optical thermometry materials is the fluorescence intensity ratio (FIR), which is based on thermally coupled energy levels (TCELs) of lanthanide ions, such as Er 3+ , Tm 3+ , and Ho 3+ . FIR shows some advantages over others, particularly, it is intrinsically self-referenced and has negligible signal drift only because the FIR value is independent of excitation power and doping concentration.…”
Section: Introductionmentioning
confidence: 99%
“…These impurity levels can be combined with excited electrons to become hole traps to generate fluorescence, and thus improve the luminosity intensity. The replacement of O 2− with a certain amount of F − ions could improve the energy transfer efficiency from the GOS host material to Tb 3+ , and contribute to the resulting Tb 3+ fluorescent transition [ 35 , 36 ]. However, with the increase in the amount of F − ions, new intrinsic defects will be formed, which will lead to a reduction in the energy transfer efficiency and emission intensity [ 37 ].…”
Section: Resultsmentioning
confidence: 99%