Elsevier

Materials Chemistry and Physics

Volume 211, 1 June 2018, Pages 181-191
Materials Chemistry and Physics

Near UV excited SrAl2O4:Dy3+ phosphors for white LED applications

https://doi.org/10.1016/j.matchemphys.2018.02.025Get rights and content

Highlights

  • SrAl2O4:Dy3+ phosphors were crystallized into monoclinic structure.

  • Upon 350 nm excitation, the SrAl2O4:Dy3+ phosphors exhibit intense luminescence.

  • The dipole-dipole interaction mechanism is responsible for luminescence quenching.

  • The SrAl2O4:1.0 mol% Dy3+ phosphor is the best choice to design white LEDs.

Abstract

Strontium aluminate phosphors containing different concentrations of Dy3+ ions (SrAl2O4:Dy3+) were prepared by solid state reaction method by sintering at 1100 °C for 3 h. These phosphors were crystallized into monoclinic structure and well consistent with the JCPDS No. 34−0379. All these phosphors exhibit the characteristic emission transitions such as 4F9/2 → 6H15/2, 4F9/2 → 6H13/2 and 4F9/2 → 6H11/2 corresponding to blue (∼480 nm), yellow (∼572 nm) and red (∼663 nm) regions when excited at 350 nm near UV wavelength. Beyond 1.0 mol% concentration of Dy3+ ions, a luminescence quenching was noticed and it has been assigned to the energy transfer through dipole-dipole interactions at higher concentrations. Due to crystallization into nanophase, the SrAl2O4:Dy3+ phosphors exhibit novel and excellent luminescence properties at 350 nm excitation. The 1.0 mol% of Dy3+ -doped SrAl2O4 phosphor show a quantum yield of ∼9.52%. The experimental results suggest that the SrAl2O4:1.0 mol% Dy3+ phosphor could be the best choice to design white LEDs with bright and intense luminescence.

Introduction

Trivalent rare earth (RE3+) ions activated mono-phase nanophosphors attracted the researchers due to their strong absorption from VUV-to-NIR region [[1], [2], [3], [4]], high color-rendering index [5,6], environmental friendly nature [7,8], chemical stability and thermal behaviour [[9], [10], [11], [12]]. They play a vital role in different fields such as science & technology, industry and bio-medicine [[13], [14], [15]]. They find wide range of applications in lasers, flat panel displays, computers, smart-phones and light emitting devices (LEDs). The emission of white light has been achieved using blue GaN-based LED with yellow or YAG: Ce3+ or tricolor phosphors excited by UV radiation. The white LEDs designed by these methods show poor illumination and low color rendering index. Many efforts have been made to overcome these limitations to develop new and novel phosphors for white LED’s. However, there is a demand for novel and high fluorescence efficiency phosphor materials to meet the present fast growing smart technology [[16], [17], [18]].

Compared to the available phosphors, the SrAl2O4 show high luminescence efficiency and excellent optical properties owing to their strong absorption in UV region, long phosphorescence, excellent emission, high thermal stability, chemical durability and eco-friendly nature [[19], [20], [21], [22], [23]]. Diaz-Torres et al. [19] reported the enhancement in white light emission of SrAl2O4:Ce3+ phosphors by co-doping with Li+ ions synthesized by combustion technique. Green SrAl2O4:Eu2+, Dy3+ phosphors synthesized by microwave assisted co-precipitation route exhibits long afterglow photoluminescence (PL) after the removal of excitation source [20]. In order to investigate the luminescence and long lasting properties, Eu2+ and Dy3+ co-doped SrAl2O4 phosphor was synthesized via sol-gel method by L. Xiao et al. [22]. S. Chawla et al. [23] presented a broad yellow emitting SrAl2O4:Pr3+ phosphor with blue excitation for white LEDs.

Under suitable excitation, the Dy3+ ions doped phosphors emit blue, yellow and red emissions corresponding to 4F9/2 → 6H15/2, 4F9/2 → 6H13/2 and 4F9/2 → 6H11/2 transitions, respectively. Among the available Dy3+ ions activated phosphors for white LED applications [21,24,25], the SrAl2O4:Dy3+ phosphors are of interest due to their excellent spectral properties and high luminescence efficiency. Sahu et al. [26] reported the photoluminescence and mechanoluminescence properties of 1.0 mol% of Dy3+ -doped SrAl2O4 phosphor only for white light generation. The present research work explores the concentration (0 ≤ x ≤ 5.0 mol%) dependent luminescence, color purity, quantum yield and fluorescence decay of SrAl2O4:Dy3+ phosphors. The possible reasons for the luminescence quenching of Dy3+ ions at higher concentrations was discussed in detail.

Section snippets

Materials and method

Different concentrations of Dy3+ ions (x = 0, 0.1, 0.5, 1.0, 2.0 and 5.0 mol%) doped SrAl2O4 phosphors were synthesized by solid state reaction method. High-purity SrCO3 (99%), Al2O3 (99.9%), and Dy2O3 (99.99%) were used as starting chemicals. Stoichiometric amounts of these chemicals were mixed thoroughly in the presence of acetone using a pestle and agate mortar. About 1.0 wt% of B2O3 was added as flux to the homogeneous mixtures to promote the decomposition of SrCO3. These mixtures were heat

Structure and morphology

The XRD profiles of SrAl2O4: xDy3+ (0 ≤ x ≤ 5.0 mol%) phosphors are well consistent to JCPDS No. 34-0379. The addition of Dy3+ impurity in small amounts (i.e., x ≤ 5.0%) has no effect on the monoclinic structure of SrAl2O4:Dy3+ phosphors. However, the intensity of XRD peaks decrease with the increase of Dy3+ ion concentration with peak positions remains unaffected. The XRD profiles of undoped and Dy3+ -doped SrAl2O4 phosphors are illustrated in Fig. 1. The average crystallite size of SrAl2O4:Dy

Conclusions

The SrAl2O4:Dy3+ phosphors have been synthesized by solid state reaction method by sintering at 1100 °C for 3 h. These phosphors are crystallized into monoclinic SrAl2O4 structure and well consistent to the JCPDS No. 34−0379. Upon 350 nm near UV excitation, the SrAl2O4:Dy3+ phosphors exhibit 4F9/2 → 6H15/2 (480 nm), 4F9/2 → 6H13/2 (572 nm) and 4F9/2 → 6H11/2 (663 nm) transitions. Beyond 1.0 mol% concentration, the Dy3+ ions show luminescence quenching due to the ET among the excited Dy3+ ions

Acknowledgement

The author is thankful to the DST and the SAIF, IIT Madras, Chennai – 600036 for providing FT-IR analysis.

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