<p>The paper reports on the synthesis and characterisation of Ce<sup>3+</sup> activated Mg<sub>3</sub>WO<sub>6</sub> phosphor, with variable (0.5&#xa0;to 2.5 mol%) concentration of doping Ce<sup>3+</sup>. The sample is synthesised <i>via</i> the combustion method. The crystal structure is determined by the X‑ray diffraction analysis, which shows the monoclinic structure with a&#xa0;P&#xa0;1 2/c1 space group. The phosphor surface morphology is analysed by scanning electron microscopy, which shows the non-uniform particle distribution. The EDX analysis confirms the proper formation of phosphor. Photoluminescence study shows that prepared phosphor exhibits both the down- and up-conversion phenomenon. The notable peak at 275 nm is mainly due to the effective transitions from 4f ground state of Ce<sup>3+</sup> to the field-splitting levels of 5d state. The emission peak at 475 nm is mainly due to the transitions of 5d excited state to <sup>2</sup>F<sub>7/2</sub> and <sup>2</sup>F<sub>5/2</sub> ground states.</p>

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Photoluminescence studies of Ce3+ doped phosphors: down/up-conversion luminescence

  • P. N. K. Chaitanya,
  • D. Dinkar,
  • P. Indira,
  • A. S. Sai Prasad,
  • M. Sree Ramana,
  • Vikas Dubey,
  • Shireen Aman,
  • Ovica Manners,
  • K. V. R. Murthy

摘要

The paper reports on the synthesis and characterisation of Ce3+ activated Mg3WO6 phosphor, with variable (0.5 to 2.5 mol%) concentration of doping Ce3+. The sample is synthesised via the combustion method. The crystal structure is determined by the X‑ray diffraction analysis, which shows the monoclinic structure with a P 1 2/c1 space group. The phosphor surface morphology is analysed by scanning electron microscopy, which shows the non-uniform particle distribution. The EDX analysis confirms the proper formation of phosphor. Photoluminescence study shows that prepared phosphor exhibits both the down- and up-conversion phenomenon. The notable peak at 275 nm is mainly due to the effective transitions from 4f ground state of Ce3+ to the field-splitting levels of 5d state. The emission peak at 475 nm is mainly due to the transitions of 5d excited state to 2F7/2 and 2F5/2 ground states.