2022
DOI: 10.1021/acsami.2c10350
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High-Efficiency and Wavelength-Tunable Near-Infrared Emission of Lanthanide Ions Doped Lead-Free Halide Double Perovskite Nanocrystals toward Fluorescence Imaging

Abstract: Near-infrared (NIR) fluorescent materials show unique photophysical properties, which make them widely used in optical communication, night vision imaging, biomedicine, and other applications. However, the development of high-efficiency and wavelength-tunable NIR nanomaterials is still a challenge. Herein, a series of lanthanide ions doped Cs2AgIn0.99Bi0.01Cl6 double perovskite nanocrystals (DPNCs) with wavelength-tunable NIR light emission (800–1600 nm) have been synthesized. The optimal photoluminescence qua… Show more

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Cited by 27 publications
(15 citation statements)
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References 48 publications
(50 reference statements)
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“…In the case of DP:S4.1, a third component (τ 3 ∼ 373 ps) is necessary to fit the kinetic curve satisfactorily. This additional time constant in Sm 3+ -doped DP is attributed to the sensitization of Sm 3+ via a nonradiative energy-transfer pathway …”
Section: Results and Discussionmentioning
confidence: 95%
See 1 more Smart Citation
“…In the case of DP:S4.1, a third component (τ 3 ∼ 373 ps) is necessary to fit the kinetic curve satisfactorily. This additional time constant in Sm 3+ -doped DP is attributed to the sensitization of Sm 3+ via a nonradiative energy-transfer pathway …”
Section: Results and Discussionmentioning
confidence: 95%
“…This additional time constant in Sm 3+ -doped DP is attributed to the sensitization of Sm 3+ via a nonradiative energy-transfer pathway. 62 The mechanism of the luminescence process in Sm 3+ -doped Cs 2 AgInCl 6 :Bi NCs is proposed in Figure 4f based on the above observations. When Cs 2 AgInCl 6 :Bi is excited at 368 nm, Bi 3+ ions absorb the energy and further shift to STEs through nonradiative relaxation processes.…”
mentioning
confidence: 89%
“…While Figure d,e represented the interstitial doping condition and the coexistence of interstitial and substitutional doping at Sc sites, respectively. The corresponding defect formation energy ( E for ) was calculated using the following equation E normalf normalo normalr = E normalt normalo normalt ( C s 2 N a S c C l 6 + T b ) E normalt normalo normalt ( C s 2 N a S c C l 6 ) + prefix∑ n i normalΔ μ i where E tot (Cs 2 NaScCl 6 + Tb) and E tot (Cs 2 NaScCl 6 ) are the total energy for Tb 3+ -doped and undoped Cs 2 NaScCl 6 systems and μ represents the chemical potential for atoms calculated as the corresponding crystal energy per atom. The calculated E for under different conditions are graphically depicted in Figure f.…”
Section: Resultsmentioning
confidence: 99%
“…In another case, ultra-broadband light emission is observed by doping the double perovskites (DPs) with Ln 3+ ions. 173,174 Jin et al 173 discovered that Cs 2 AgInCl 6 double perovskite doping by Ln 3+ (Ln = La to Lu) and Bi 3+ shows ultra-broadband light emission ranging from 400 to 2000 nm wavelength. The Bi/Ln:Cs 2 AgInCl 6 (Ln = Er, Ho, Tm) double perovskite showed ultra-broadband continuous emission due to the 4f-4f transition of Ln 3+ ions with superior long-term stability.…”
Section: Outlook and Future Challengesmentioning
confidence: 99%