Elsevier

Optical Materials

Volume 100, February 2020, 109623
Optical Materials

Novel blue emitting Tm3+ activated lanthanum molybdate: Investigations on luminescence behaviour and Judd-Ofelt theoretical analysis

https://doi.org/10.1016/j.optmat.2019.109623Get rights and content

Highlights

  • Novel Tm3+ doped blue phosphor synthesized by a simple technique.

  • Oriented attachment mediated growth mechanism.

  • Intense sharp blue emission at 453 nm.

  • Highly asymmetric site occupancy from JO analysis.

  • CIE co-ordinates fall in blue region.

Abstract

Novel blue emitting thulium doped La2(MoO4)3 nanophosphors were synthesized by facile co-precipitation method and the spectroscopic features were systematically studied on the basis of Judd-Ofelt analysis. The tetragonal phase formation of Tm3+ doped La2(MoO4)3 with space group I41/a is confirmed from the XRD analysis and the growth mechanism by oriented attachment is revealed by TEM analysis. The 1D23F4 transition at 453 nm is the dominant emission peak of Tm3+ in the photoluminescence emission spectra and offers major contribution towards the intense blue emission of the phosphor material. The Judd-Ofelt intensity parameters exhibit the trend Ω2>Ω4>Ω6, which point out the asymmetric site occupancy of Tm3+ ions in the host matrix. The estimated higher branching ratio for 1D23F4 blue emission of Tm3+ signifies it as a potential laser emission transition. The CIE chromaticity co-ordinates of optimized La1.94Tm0.06(MoO4)3 nanophosphors falls in the blue region of the chromaticity diagram with co-ordinates (0.214,0.097).

Introduction

Multifaceted optical applications associated with rare earth luminescence are primarily devoted to their intense sharp multicolour emissions originating from 4f-4f intraconfigurational transitions. The lifting up of degeneracy in intra 4f forbidden transitions of rare earth ions by the influence of a strong crystal field offered by the host matrix is the key point of rare earth luminescence [1,2]. Obviously, solid state lighting technology demands highly efficient NUV or blue LED excitable red, green and blue phosphors with high efficiency and colour purity. Nowadays tremendous works are reported on Tb3+ and Eu3+ based green and red phosphors with desirable properties [[3], [4], [5], [6], [7], [8]]. However, the spectroscopic investigation on blue emitting phosphors is relatively less and most of them are characterized with broad blue emission bands. Foka et al. reported the photoluminescence studies on Ce3+ activated SrAl2O4 and Tabaza et al. reported Ce3+ activated MgAl2O4, which are UV excitable blue phosphors [9,10]. A broad emission band in the range 340–440 nm and a broad blue-green emission band centered at 490 nm were observed for Ce3+ activated SrAl2O4 and MgAl2O4 phosphors respectively. Pawade et al. synthesized Eu2+ doped SrMg2Al16O27 blue phosphors with a broad excitation band centered at 324 nm and a broad emission band with a maximum at 465 nm [11]. Eu2+ doped Ca2Sr(PO4)2 blue phosphor with a broad excitation band in the range 200–410 nm and a broad emission band in the range 410–500 nm with a maximum at 430 nm were synthesized and characterized by X. Wang et al. [12]. Another blue phosphor which is used in plasma display panels is Tm3+ activated lanthanum phosphate [13]. The material is excited either at 147 or 173 nm and the emission peaks are observed at 348, 362 and 452 nm.

Most of the blue emitting phosphors discussed above possess a broad emission band in the blue region. The advantage of Tm3+ activated phosphors is that, instead of a broad band, intense sharp peaks are observed in the blue region corresponding to the emission from 1D2 and 1G4 emitting levels. The sharp emission due to f-f transitions in Tm3+ ions is beneficial for enhancing the spectral purity of blue emission, compared with other broad band blue emitters. In addition, as these emitting levels are well separated from the next lower lying levels of Tm3+ ions, the possibility of non-radiative processes from these states through multiphonon relaxation is less, even in high phonon energy host matrices. Also, the sharp excitation peak of Tm3+ observed at 360 nm facilitates efficient UV excitation of the material. On account of all these facts, luminescence properties of Tm3+ based blue phosphors deserve much attention. The origin of blue emission of Tm3+ is attributed to 1D23F4 and 1G43H6 transitions corresponding to 453 and 473 nm emissions respectively [14,15]. The Tm3+ emission is highly sensitive to the nature of the host lattice in which they are embedded. There are few reports on the Tm3+ based luminescence in tungstate, molybdate and vanadate host lattices. L. Guerbous et al. reported host sensitized Tm3+ luminescence in LiIn(WO4)2 phosphors and J. Liao et al. investigated the spectroscopic and the morphological aspects of AWO4 (A = Ca,Sr,Ba) blue phosphors [15,16]. The synthesis and the photoluminescence properties of Tm3+ doped YxGd1-xVO4 nanophosphors were studied by B.Yan et al. [14]. Likewise, the spectroscopic properties on the basis of Judd-Ofelt theoretical analysis of Tm3+ doped NaBi(MoO4)2 single crystals were carried out by N.V. Gusakova et al. [17]. D. Zhu et al. synthesized Tm3+/Dy3+ co-doped BamSr1−mMoO4 polycrystals by a low temperature combustion method and investigated the luminescence properties of the material for the realization of white light generation [18].

Molybdate based crystals are proved to be one of the excellent host matrices for the incorporation of rare earth ions. They are self activated luminescent materials with strong absorption in the UV region and efficient energy transfer to the dopant ions via Mo–O charge transfer band absorption [19]. In addition, they have high thermal and chemical stability [20]. Generally, nanophosphors with superior emission properties synthesized by simple cost-effective synthesis technique deserve much attention. In the present work, lanthanum molybdate which is an outstanding candidate for the incorporation of luminescent rare earth ions is chosen as the host lattice and investigated the spectroscopic properties of the material. The detailed investigations on the Tb3+ doped green phosphors and the tunable dual colour emitting Tb–Eu co-doped La2(MoO4)3 nanophosphors via energy transfer mechanism were reported in our previous works [21,22].

The synthesis and characterization of Tm3+ activated lanthanum molybdate nanophosphors and the JO analysis is reported for the first time. The technique adopted for the synthesis is a simple and cost-effective method. Due to the asymmetric site occupancy of Tm3+ in tetragonal La2(MoO4)3 host, electric dipole transition will dominate and thus maximum emission intensity is assured for purely electric dipole blue emission transition of Tm3+ ions. Apart from the photoluminescence investigations, the studies are extended towards colorimetric analysis in order to get a complete picture of the emission properties of the material. In addition, there are no previous reports on JO analysis and the prediction of radiative parameters of Tm3+ activated La2(MoO4)3 host matrix. Almost all the previous studies on Tm3+ doped in different matrices were solely concentrated on the optical characterizations and lacks morphological investigations [16,23]. However, in the present study the morphological features of the material were also investigated.

Section snippets

Materials and synthesis

In a typical synthesis process Lanthanum (III) nitrate hexahydrate [La(NO3)3.6H2O, Alfa Aesar, 99.9%], Thulium (III) nitrate pentahydrate [Tm(NO3)3.5H2O, Sigma Aldrich, 99.9%] and Sodium molybdenum oxide dihydrate (Na2MoO4.2H2O, CDH, 99%) were used as the starting materials. The La2-xTmx(MoO4)3 samples were prepared by conventional co-precipitation method and the detailed procedure followed in the synthesis were included in our previous report [21]. A set of La2-xTmx(MoO4)3 samples with varying

Characterizations

The Rigaku RU-200B X-ray powder diffractometer with nickel filtered Cu Kα radiation (λ = 1.5406 Å) recorded the X-ray diffraction patterns. The detailed morphological features of the samples were studied using Transmission Electron Microscopy (TEM) and High-Resolution Transmission Electron Microscopy (HRTEM) micrographs recorded on a JEOL JEM 2100 transmission electron microscope. The Carl Zeiss EVO 18 Secondary Electron Microscope with AMETEK EDAX Octane series attachment was used for Energy

Crystal structure and XRD analysis

The scheelite-type crystal with chemical formula La2(MoO4)3 crystallizes in tetragonal symmetry with a space group I41/a and the crystal structure is sketched in Fig. 1. There are eight oxygen atoms around La3+ cations, which are arranged such that a trigonal dodecahedron unit is formed and the individual units are interconnected through common edges. Similarly, the Mo6+ cation in the structure is surrounded by four oxygen atoms forming a distorted tetrahedra and each of the (MoO4)2- units are

Conclusions

Blue emitting Tm3+ doped lanthanum molybdate nanophosphors were synthesized by facile co-precipitation method. Primary particles of size 20–40 nm were identified from TEM analysis and nanoparticles exhibit a tendency to attach with each other to form elongated structures by means of oriented attachment mechanism. The prominent blue emission of the nanophosphors is attributed to 1D23F4 transition of Tm3+ ions. The La1.94Tm0.06(MoO4)3 nanophosphors exhibit highest luminescence intensity and is

Author contributions

Kukku Thomas: Research Scholar, who carried out the synthesis and characterization of the materials, analyzed the data and interpreted the results and prepared the manuscript.

Dinu Alexander: Assisted in the JO analysis.

Linju Ann Jacob: Assisted in the morphological analysis.

P R Biju: Co-supervisor of the work. Assisted in all aspects.

N V Unnikrishnan: Assisted in PL studies.

Cyriac Joseph: Research supervisor. Suggested the concept of the work and guided in the entire work.

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.

Acknowledgements

This work is financially supported through SAP-DRS (No. F.530/12/DRS/2009 (SAP-1)) and DST-PURSE (SR/417 & 418/2017) programs. The author Kukku Thomas is grateful to University Grants Commission, Govt. of India for the award of MANF fellowship. Dinu Alexander is thankful to University Grants Commission, Govt. of India for the award of RFSMS fellowship. Linju Ann Jacob is thankful to UGC, Govt. of India for the financial assistance through the scheme of faculty development program (FDP).

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