Synthesis, optical properties, and packaging of Dy3+ doped Y2WO6, Y2W3O12, and Y6WO12 phosphors

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Highlights

  • Y2WO6, Y2W3O12, and Y6WO12 were synthesized.

  • The Dy3+ doped Y2WO6 has the strongest PL intensities.

  • The Dy3+ optimal doping concentration was 2 mol% in Y2WO6 phosphor.

  • 2 mol% Dy3+ doped Y2WO6 phosphor kept 74 % intensity of 50 °C at 150 °C.

  • WLEDs were obtained by combining the phosphor with 308 nm chips.

Abstract

Through a solid-state reaction method, Dy3+ doped monoclinic phase of Y2WO6, Y2W3O12, and hexagonal phase of Y6WO12 phosphors were synthesized. The Y2WO6 and Y2W3O12 were composed of micrometre-scale particles, and the Y6WO12 was composed of nanometre particles. The energy-dispersive spectra (EDS) suggested that the atom ratio of Y to W decreased with the sequence of Y6WO12, Y2WO6, and Y2W3O12 phosphors. The Eg values were calculated based on the diffuse reflection (DR) spectra. The Dy3+ doped Y2WO6 phosphor had the most intense photoluminescence (PL) intensities and the optimal doping concentration was 2 mol%. The energy transfer efficiency from WO66− to Dy3+ was calculated. The lifetime of 4F9/26H13/2 transition of Dy3+ was a few hundred nanoseconds. At 150 °C, the 2 mol% Dy3+ doped Y2WO6 phosphor kept 74 % intensity of 50 °C. The white light emitting diode (WLED) devices were fabricated by combining phosphors with 308 nm LED chips.

Graphical abstract

PL excitation and emission spectra of Dy3+ doped Y2WO6, mixture of Y2WO6 and Y2W3O12, Y2W3O12, and Y6WO12 phosphors.

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Introduction

Owing to its applications in white light, laser emissions, temperature sensing, etc., rare earth ion Dy3+ has received attractive attentions [[1], [2], [3], [4], [5], [6]]. The Dy3+ has characteristic emissions originated from the 4F9/26H15/2 transition located at blue area and the 4F9/26H13/2 transition located at yellow region. In general, there are two methods being used and explored to obtain phosphor converted white-light-emitting diodes (WLEDs). One is combining a blue-emitting chip with yellow phosphor (usually Ce3+ doped yttrium aluminum garnet YAG). The other is packaging red, green and blue phosphors together to an ultraviolet (UV) chip. For the Dy3+ has blue and yellow emissions simultaneously, it is expected that white emission can be obtained in Dy3+ single doped phosphors [7,8].

It is well known that the tungstate is a kind of self-activated phosphor and can produce a broad band emission under UV excitation [9]. In general, metal tungstates can be divided into two groups based on the coordination environment around the tungsten. One group is regular WO42− tetrahedra with scheelite-type structure [10,11]. The other group is six-fold coordinated distorted WO66- octahedra with wolframite-type structure [12]. RE2WO6 (rare earth = RE) tungstates have the wolframite-type structure. The charge transfer band (CTB) of WO66- usually locates at around 300 nm. The energy transfer process from the WO66- group to RE3+ can happen and intense luminescence of RE-doped tungstates can be obtained [13]. Color-tunable emissions in Sm3+, Eu3+, Tb3+, Dy3+ doped Y2WO6 or Y6WO12 have been reported and researched [[14], [15], [16], [17], [18], [19]]. Rarely reports on other yttrium tungsten oxides were reported [20]. Some yttrium tungsten oxide phosphors of Dy3+ doped Y2WO6, Y2W3O12, and Y6WO12 were synthesized by a solid-state reaction method. The obtained materials were characterized by crystalline structures, particle sizes and compositions, energy transfer processes, energy transfer efficiencies, optical properties, and thermal stabilities, et al. The obtained 2 mol% Dy3+ doped Y2WO6 phosphor was packaged into WLED devices and gave bright white light under forward bias.

Section snippets

Experimental section

Dy3+ doped yttrium tungsten oxide phosphors were synthesized using the same solid-state reaction method as reported in ref. [21]. Tungsten oxide (WO3, A.R.) were used to replace molybdenum trioxide (MoO3, 99.99 %), yttrium oxide (Y2O3, 99.99 %) were used to replace lutetium oxide (Lu2O3, 99.99 %), and dysprosium oxide (Dy2O3, 99.99 %) were used to replace europium oxide (Eu2O3, 99.99 %) as raw materials. For the synthesis of 1, 2, 4, 6, and 10 mol% Dy3+ doped Y2WO6 phosphors, stochiometric of Dy

Structural analysis

Fig. 1 presents XRD patterns of materials synthesized with different ratios of Y(Dy)2O3 to WO3. The reference data are also illustrated in Fig. 1. With molar ratio of Y(Dy)2O3:WO3  = 1:1 and fixed Y2O3:Dy2O3 = 99:1 in molar ratio, the obtained XRD pattern can be well indexed to the reference data of monoclinic phase of Y2WO6 with JCPDS card 23-1489, which suggests that the Dy3+ doped monoclinic phase of Y2WO6 was obtained. With the molar ratio of Y(Dy)2O3:WO3 = 1:2, some peaks marked * can be

Conclusion

In conclusion, the Dy3+ doped monoclinic phase of Y2WO6, Y2W3O12, hexagonal phase of Y6WO12, and undoped Y2WO6 phosphors were synthesized through a solid-state reaction method. The FE-SEM images suggests that the materials were composed of micrometre particles except Y6WO12 phosphor. The EDS patterns confirmed the compositions of the materials. The DR spectra consisted well with the PL excitation spectra and the Eg values were deduced from the DR spectra. The results suggested that the Dy3+

CRediT authorship contribution statement

Chunyan Cao: Conceptualization, Methodology, Writing - original draft, Writing - review & editing, Project administration, Funding acquisition. Shoujin Wei: Formal analysis, Investigation. Yongxing Zhu: Formal analysis, Investigation. Tao Liu: Formal analysis, Investigation. An Xie: Methodology, Supervision. Hyeon Mi Noh: Project administration. Jung Hyun Jeong: Project administration, Funding acquisition.

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.

Acknowledgments

The research work was supported by the Natural Science Foundation of Fujian Province (Grant nos. 2017J01719, 2018J01429), Fujian Key Laboratory of Functional Materials and Application open projects (Grant nos. fma2017106, fma2018001), Pandengketi of Xiamen University of Technology (XPDKT19038), and Program for Innovative Research Team in Science and Technology in Fujian Province University (IRTSTFJ). This research was also supported by Basic Science Research Program through the National

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