Mn2+ ions substitution inducing improvement of optical performances in ZnAl2O4: Cr3+ phosphors: Energy transfer and ratiometric optical thermometry

https://doi.org/10.1016/j.saa.2021.120321Get rights and content

Highlights

  • ZnAl2O4 without inversion defects are fabricated through doping with Mn2+.

  • Red emission is enhanced about 15.8 times in ZnAl2O4 crystals doped with Mn2+ ions.

  • The mechanism composited of energy transfer and reducing inversion defects is present.

  • The higher sensitivity for optical thermometry is obtained.

Abstract

Zn1-xMnxAl2O4:0.1 mol% Cr3+ (0.04x0.16) phosphors with single spinel phase were synthesized by using sol–gel method and the structure, optical and temperature sensing performances were reported herein. The results of X-ray photoelectron spectra indicate that the inversion defects related to octahedral Zn are reduced and the crystal field surrounding Al changes with Mn2+ doping in ZnAl2O4 lattices. Mn2+/Cr3+ co-doped ZnAl2O4 nanophosphors reveal a green emission band assigned to Mn2+ and a series of red emission peaks assigned to Cr3+, respectively. With the concentration of Mn2+ increasing, the intensity of zero phonon line (R line) assigned to Cr3+ increases, reaching the maximum at the optimal Mn2+ concentration of x=0.14. The energy transfer from Mn2+ to Cr3+ is confirmed with the energy transfer efficiency of 83%. The separation between 2E(eg) and 2E(tg) of Cr3+ is enlarged due to Mn2+ dopants giving rise to a change of crystal field. The luminous intensity ratio between two separated emission peaks at 685 nm (R3) and 689 nm (R2) reveals an obvious temperature dependence. The relative sensitivity changes from 3.7 %K−1 to 0.25 %K−1 with the temperature increasing from 80 K to 310 K, which is much larger than that of ZnAl2O4:Cr3+ nanophosphors without Mn2+, indicating its good application prospect in optical thermometry.

Introduction

Temperature measurement is a basic and vital subject in agricultural and industrial manufacture, biology and personal daily life. Most of temperature measurement technologies require physical contact commonly, while noncontact temperature measurement is desired in numerous fields such as biological imaging, industrial manufacture, environment monitoring and so on[1], [2], [3]. Optical thermometry has been attracted more attentions due to its high spatial resolution, high detection sensitivity and rapid response in noncontact measurement process[4], [5], [6]. In many types of optical thermometers, the temperature sensing based on fluorescence intensity ratio (FIR) has been widely investigated recently due to its significant accuracy and reliability. The performance of temperature sensing can be evaluated by the relative sensitivity (Sr) which can be improved by optimizing the matrix materials and dopants[7], [8], [9], [10]. Most investigations are focused on the rare earth (RE) doped variety of host lattices due to their excellent optical performances and stable energy level transition, e.g. Ho3+-doped Na0.5Bi0.5TiO3 ceramics (Sr = 1.03 %@377 K, 6.14 %@167 K)[11], Er3+-doped SrLaAlO4 phosphors (Sr = 1.42 %K−1@298 K)[12], Tm3+ and Yb3+ co-doped LiNbO3 single crystal[13], Eu3+, Tb3+ co-doped Gd2(MoO4)3 phosphors[14], and so on, have been reported recently.

While the expensive price of RE limits their application. Transition metals have been considered as the alternatives of RE due to their excellent optical properties and popular price[1], [15]. Some transition elements, such as Mn, Cr and so on, exhibit obvious temperature dependence of photoluminescence. Zhu et al. [16] reported the high sensitivity optical thermometry of Mn2+/Mn4+ co-doped BaAl12O19/SrAl12O19 system with the relative sensitivity of 4.37 % %K−1@293 K. The FIR property of Mg2TiO4:Mn4+ phosphor with relative sensitivity of 0.0254 %K−1[17] and Sn2+/Mn2+ co-doped Sr2P2O7 phosphor with relative sensitivity of 0.027 %K−1[18].

Comparing to the Mn ions, Cr3+ has the more chemical stability, thus attracts more attentions recently. In the host materials with strong crystal field, the emission assigned to the transition from the 2E state to 4A2 (ground state) is dominated, and the 2E level splits into 2E(E¯) and 2E(2A¯) levels due to Cr3+ replacing the Al3+ in distorted octahedral sites, giving rise to two lines of R1 (2E(2A¯)4A2, 687 nm) and R2 (2E(E¯)4A2, 689 nm), as shown in Fig. 1 (a). The N-lines are assigned to Cr3+ in the inversion defects environment. The luminous characteristics of Cr3+ are strongly affected by the thermal quenching effects and crystal field[19], [20], thus the temperature dependence of fluorescence intensity ratio, lifetime, emission wavelength is suitable for optical thermometry, and the feasibility of Cr-doped luminescence sensors for luminescence thermometry has been investigated in various materials, such as ZnGa2O4[21], Al2O3[22], YAlO3[23], MgAl2O4[24], BeAl2O4[25] and so on. The Ueda et al. investigated the temperature dependence of the photoluminescence (PL) spectrum of Cr3+ doped ZnGa2O4, and reported the temperature measurement performance based on the fluorescence intensity ratio between 4T24A2 to 2E→4A2 luminescence bands with a high Sr of 2.8 %/K at 310 K[26]. Glais et al. reported an optical thermometer of Cr and Bi co-doped ZnGa2O4 phosphors with the Sr of 1.7 %/K at 190 ℃[21]. However, the emission band assigned to 4T24A2 transition is difficult to observe at low temperatures in ZAO crystals. Furthermore, the emissions related to N lines, Stokes and Anti-Stokes reveal wide and overlap spectra and reveal same change trend with temperature decreasing, so it is difficult to confirm the integral intensity accurately. When Mn2+ enters zinc aluminate lattices, the crystal field surrounding Cr3+ should be changed, and gives rise to the 2E(2A¯) level shifting furtherly, which results in a new emission (R3 line) assigned to Cr3+ as shown in Fig. 1(b). It is interesting to investigate whether R3 line is considered as a new reference signal.

In this paper, Mn2+/Cr3+ co-doped ZnAl2O4 (ZAO) phosphors were fabricated by common sol–gel method. The energy transfer process from Mn2+ to Cr3+ has been investigated with various concentrations of Mn2+. With the concentration of Mn2+ increasing, the reversion defects are reduced and the separation between 2E(E¯) and 2E(2A¯) level splits furtherly. The relative intensity of N lines assigned to Cr3+ surrounded inversion defects in spinel lattices is reduced, as well as the Stocks and anti-Stocks lines become weaker. The temperature dependence of photoluminescence spectra of Mn2+ and Cr3+ co-doped ZnAl2O4 phosphors reveals better temperature sensitivity than that of Cr3+ single doped ZnAl2O4 phosphors, indicating the potential application in optical thermometry.

Section snippets

Experimental details

The precursor materials were aluminate nitrate nonahydrate (Al(NO3)3·9H2O), zinc nitrate hexahydrate (Zn(NO3)2·6H2O), chromium chloride hexahydrate (CrCl3·6H2O), manganese acetate tetrahydrate (Mn(CH3COO)2·4H2O) and ethylene glycol (EG).

Zn, Mn and Al were taken in the molar ratio (1-x): x: 2, where x = 0, 0.02, 0.04, 0.06, 0.08, 0.10, 0.12, 0.14, 0.16, and the molar ratio between Al and Cr is 1000:1 for all the samples. Zn1-xMnxAl2O4:Cr3+ phosphors were synthesized by using sol–gel method as

Structural characterization

The crystal structure of Zn1-xMnxAl2O4:Cr3+ phosphors is characterized by XRD, and the results are shown in Fig. 2(a). Single spinel phase is formed for all samples even doped with Mn concentration of x=0.16. With the Mn concentration increasing, the intensity of diffraction peaks is reduced, but the full width at half maximum (FWHM) decreases. The crystallinity can be evaluated by using mean crystalline size which is estimated by Scherrer’s equation as following expression[29]:D=0.9λFWHMcosθ

Conclusions

In summary, Mn2+ and Cr3+ co-doped ZnAl2O4 phosphors were fabricated by using common sol–gel method. Mn2+ ions were introduced into the spinel lattices to tune the local crystal field of the activators. Due to the same valence with that of Zn2+ ions, zinc aluminate crystals still revealed pure spinel phase with Mn2+ concentration increasing from 0 to 16 mol%. An efficient energy transfer process from Mn2+ to Cr3+ is observed monitoring at 427 nm of the excitation wavelength, and it played an

CRediT authorship contribution statement

Bingjun Zhu: Formal analysis, Investigation, Writing – original draft, Visualization. Naizhen Li: Investigation, Formal analysis. Shiqi Ren: Investigation, Visualization. Yunlong Liu: Data curation. Dong Zhang: Conceptualization, Methodology, Validation, Resources, Writing – original draft, Writing – review & editing, Supervision, Project administration. Qingru Wang: Validation, Methodology. Qiang Shi: Data curation. Qinglin Wang: Validation. Shuhong Li: Data curation. Bingyuan Zhang:

Declaration of Competing Interest

The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

Acknowledgement

This work was supported by Initial Foundation for Doctor Project of Liaocheng University (No. 318051410, 318012016), the National Natural Science Foundation of China (Grant No. 61775089), the Shandong Province Natural Science Foundation of China (Grant No. ZR2018MA036, ZR2019MF068, ZR201910210137), Industrial Alliance Fund of Shandong Provincial Key Laboratory (Grant No. SDKL2016038), ‘Taishan Scholars’ Construction Special Fund of Shandong Province, Science and Technology Plan of Youth

References (45)

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