2022
DOI: 10.1002/anie.202206437
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Ultra‐Sensitive, Selective and Repeatable Fluorescence Sensor for Methanol Based on a Highly Emissive 0D Hybrid Lead‐Free Perovskite

Abstract: A convenient and rapid detection method for methanol in ethanol remains a major challenge due to their indistinguishable physical properties. Herein, a novel fluorescence probe based on perovskite was successfully designed to overcome this bottleneck. We report a new zero‐dimensional (0D) hybrid perovskite of [MP]2InxSb1−xCl7 ⋅ 6 H2O (MP=2‐methylpiperazine) displaying an unusual green light emission with near‐unity photoluminescence quantum yield. Remarkably, this 0D perovskite exhibits reversible methanol‐res… Show more

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Cited by 92 publications
(37 citation statements)
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“…This implies that the Mn 2+ doping improves the thermodynamic stability of Cs 7 Cd 3 Br 13 significantly, which agrees well with the above theoretical calculation. Moreover, the FWHM of both emission bands becomes slightly larger, and the blue STE2 emission band presents a significant red shift as the temperature increases, which is ascribed to the enhanced electron–phonon interaction caused by the strong lattice distortion at elevated temperatures. In contrast, the orange emission band composed of STE1 from Cs 7 Cd 3 Br 13 and Mn 2+ (d–d) transition exhibits a slight blue shift with the temperature increasing. To shed light on the substantial mechanism responsible for this phenomenon, the temperature-dependent PL spectra of Cs 7 Cd 3 Br 13 and Cs 7 Cd 3 Br 13 :12%Mn 2+ are measured separately.…”
Section: Resultsmentioning
confidence: 98%
“…This implies that the Mn 2+ doping improves the thermodynamic stability of Cs 7 Cd 3 Br 13 significantly, which agrees well with the above theoretical calculation. Moreover, the FWHM of both emission bands becomes slightly larger, and the blue STE2 emission band presents a significant red shift as the temperature increases, which is ascribed to the enhanced electron–phonon interaction caused by the strong lattice distortion at elevated temperatures. In contrast, the orange emission band composed of STE1 from Cs 7 Cd 3 Br 13 and Mn 2+ (d–d) transition exhibits a slight blue shift with the temperature increasing. To shed light on the substantial mechanism responsible for this phenomenon, the temperature-dependent PL spectra of Cs 7 Cd 3 Br 13 and Cs 7 Cd 3 Br 13 :12%Mn 2+ are measured separately.…”
Section: Resultsmentioning
confidence: 98%
“…In addition, the degree of the deformation of a single [Pb−Cl 6 ] octahedron can be quantitatively assessed with the following equations for the octahedral angular variance σ 2 and distortion parameter Δ d When subjected to thermal stimulation, the (TPA)PbCl 3 -Green and (TPA)PbCl 3 -Blue octahedral structure of the ground state undergoes varying degrees of deformation, which may result in the structure of the excited states being somewhat different, giving them varied Stokes shifts. 10 To further determine the origin of emission, temperature-dependent PL spectra of (TPA)PbCl 3 -Green are recorded (Figure S13). With increasing temperature, the PL peak position shows minor redshifts accompanied by gradually increasing fluorescence intensity, which has been reported in (TPA) 2 PbBr 4 .…”
Section: ■ Results and Discussionmentioning
confidence: 99%
“…The larger values of Δ d and σ 2 normally represent greater degrees of octahedral distortion. When subjected to thermal stimulation, the (TPA)­PbCl 3 -Green and (TPA)­PbCl 3 -Blue octahedral structure of the ground state undergoes varying degrees of deformation, which may result in the structure of the excited states being somewhat different, giving them varied Stokes shifts . To further determine the origin of emission, temperature-dependent PL spectra of (TPA)­PbCl 3 -Green are recorded (Figure S13).…”
Section: Resultsmentioning
confidence: 99%
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“…In addition, 0-D IOMHs may own soft lattice and strong electron–phonon coupling, thus leading to interesting photoluminescent properties, including broad emission and large Stokes shift [ 10 ]. As a result, the applications of photoluminescent 0-D IOMHs have flourished in light-emitting diode [ 11 , 12 , 13 , 14 , 15 ], X-ray scintillator [ 16 , 17 , 18 ], remote thermography [ 19 , 20 ], optical waveguide [ 21 ], anti-counterfeiting [ 22 , 23 , 24 , 25 , 26 ], as well as sensor [ 27 , 28 , 29 , 30 ].…”
Section: Introductionmentioning
confidence: 99%