2018
DOI: 10.1039/c7tc05796b
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Er3+/Yb3+ codoped phosphor Ba3Y4O9 with intense red upconversion emission and optical temperature sensing behavior

Abstract: Bright red upconversion phosphor Ba3Y4O9:Er3+/Yb3+ and dual-color complementary optical thermometry to maintain relatively high sensitivities over a wide temperature scope.

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Cited by 118 publications
(51 citation statements)
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“…[ 101,102 ] However, there is no clear or systematic strategy for selecting appropriate host matrixes as luminescence thermometers with desired thermometric performance, and tremendous efforts have been devoted to figuring it out in the past few years, especially in 4 S 3/2 / 2 H 11/2 TCL‐based thermometers. [ 103–105 ] In this part, the effect of host materials on thermal sensitivity should be demonstrated using same TCLs with similar energy gaps to exclude the impact of ∆E , thus 4 S 3/2 / 2 H 11/2 TCLs of Er 3+ are mainly discussed as an illustrative example. As mentioned above, the crystal‐field Hamiltonian used for calculating Er 3+ energy level diagram could be regarded as a perturbation of the free‐Er 3+ Hamiltonian, leading to a little fluctuation of S r value and energy gap between 4 S 3/2 / 2 H 11/2 in most of host matrices.…”
Section: Influential Factors On Thermal Sensitivitymentioning
confidence: 99%
“…[ 101,102 ] However, there is no clear or systematic strategy for selecting appropriate host matrixes as luminescence thermometers with desired thermometric performance, and tremendous efforts have been devoted to figuring it out in the past few years, especially in 4 S 3/2 / 2 H 11/2 TCL‐based thermometers. [ 103–105 ] In this part, the effect of host materials on thermal sensitivity should be demonstrated using same TCLs with similar energy gaps to exclude the impact of ∆E , thus 4 S 3/2 / 2 H 11/2 TCLs of Er 3+ are mainly discussed as an illustrative example. As mentioned above, the crystal‐field Hamiltonian used for calculating Er 3+ energy level diagram could be regarded as a perturbation of the free‐Er 3+ Hamiltonian, leading to a little fluctuation of S r value and energy gap between 4 S 3/2 / 2 H 11/2 in most of host matrices.…”
Section: Influential Factors On Thermal Sensitivitymentioning
confidence: 99%
“…Two main emissions located at 525 and 545 nm are ascribed to 2 H 11/2 → 4 I 15/2 and 4 S 3/2 → 4 I 15/2 transitions of Er 3+ , respectively . Three weak peaks located at 605, 625, and 650 nm are ascribed to ( 2 D, 2 P) 3/2 → 4 G 11/2, 4 G 11/2 → 4 I 11/2 and 4 F 9/2 → 4 I 15/2 transitions of Er 3+ , respectively . Moreover, it is quite obvious that the Gd 2 (WO 4 ) 3 :Er,Yb@SiO 2 phosphors are more feasible for further research because of their higher luminescent intensity.…”
Section: Resultsmentioning
confidence: 99%
“…However, definitely, in this work, this pair of thermally coupled levels is hard to apply to temperature sensing because of the weak green UC emission. Actually, the thermally coupled red Stark sublevels of Er 3+ 4 F 9/2 manifold can also be employed to measure the temperature with perfect sensitivity …”
Section: Resultsmentioning
confidence: 99%
“…Actually, the thermally coupled red Stark sublevels of Er 3+ 4 F 9/2 manifold can also be employed to measure the temperature with perfect sensitivity. 30,31 Subsequently, in order to investigate the temperature sensing behavior based on the thermally coupled red Stark sublevels, the thermal evolution red UC emission spectra of CaO-Y 2 O 3 : 10% Yb 3+ /4% Er 3+ were measured and are shown in Figure 4. There are several emission peaks existing in the range of 600-700 nm, which belong to the Stark transitions of 4 F 9/2 → 4 I 15/2 transition.…”
Section: The Optical Thermometry Behaviors Of Cao-y 2 O 3 : Yb 3+ /mentioning
confidence: 99%