2022
DOI: 10.1021/acs.jpclett.1c04000
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Highly Sensitive Dual-Mode Optical Thermometry of Er3+/Yb3+ Codoped Lead-Free Double Perovskite Microcrystal

Abstract: In this Letter, erbium (Er 3+ ) and ytterbium (Yb 3+ ) codoped perovskite Cs 2 Ag 0.6 Na 0.4 In 0.9 Bi 0.1 Cl 6 microcrystal (MC) is synthesized and demonstrated systematically to the most prospective optical temperature sensing materials. A dual-mode thermometry based on fluorescence intensity ratio and fluorescence lifetime provides a self-reference and highly sensitive temperature measurement under dual wavelength excitation at a temperature from 300 to 470 K. Combined with the white-light emission derived … Show more

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Cited by 56 publications
(27 citation statements)
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“…, where dFIR denotes the uncertainty on the FIR estimation. 17,27 The calculated minimum value of dT shown in Considering the discrepant trends of green and red emission intensities with the increasing temperature, construction of a FIR strategy referring to the 2 H 11/2 and 4 F 9/2 levels of Er 3+ , termed as NTCEL, 42 is also significant for the temperature readout. The values of FIR (I 536nm /I 660nm ) can be well fitted via the polynomial formula: 15,42…”
Section: Resultsmentioning
confidence: 99%
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“…, where dFIR denotes the uncertainty on the FIR estimation. 17,27 The calculated minimum value of dT shown in Considering the discrepant trends of green and red emission intensities with the increasing temperature, construction of a FIR strategy referring to the 2 H 11/2 and 4 F 9/2 levels of Er 3+ , termed as NTCEL, 42 is also significant for the temperature readout. The values of FIR (I 536nm /I 660nm ) can be well fitted via the polynomial formula: 15,42…”
Section: Resultsmentioning
confidence: 99%
“…Considering the discrepant trends of green and red emission intensities with the increasing temperature, construction of a FIR strategy referring to the 2 H 11/2 and 4 F 9/2 levels of Er 3+ , termed as NTCEL, 42 is also significant for the temperature readout. The values of FIR ( I 536nm / I 660nm ) can be well fitted via the polynomial formula: 15,42 FIR = A 3 T 3 + A 2 T 2 + A 1 T + A 0 where A 3 , A 2 , A 1 and A 0 represent the fitting constants. The fitting results are exposed in Fig.…”
Section: Resultsmentioning
confidence: 99%
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