2018
DOI: 10.1016/j.jpcs.2018.01.031
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Orange-red emitting Gd2Zr2O7:Sm3+: Structure-property correlation, optical properties and defect spectroscopy

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Cited by 37 publications
(11 citation statements)
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“…The short one is attributed to Eu 3+ ions occupying the distorted HfO 6 octahedra, whereas the long one is attributed to Eu 3+ ions occupying the highly symmetric GdO 8 site. Eu 3+ ions also exhibited biexponential decay in other pyrochlore hosts such as La 2 Hf 2 O 7 , Gd 2 Zr 2 O 7 , and Nd 2 Zr 2 O 7 wherein one of the lifetimes is attributed to A 3+ site occupancy and other to B 4+ site occupancy. , Normally, the short lifetime is attributed to asymmetric environment as f–f transition becomes relaxed, and the long lifetime is mostly attributed to symmetric environment as f–f transition is La Porte forbidden. , The biexponential behavior can also arise due to other reasons such as the presence of defects, energy transfer, and so forth. This phenomenon has been substantiated with theoretical calculations in the next section.…”
Section: Results and Discussionmentioning
confidence: 99%
“…The short one is attributed to Eu 3+ ions occupying the distorted HfO 6 octahedra, whereas the long one is attributed to Eu 3+ ions occupying the highly symmetric GdO 8 site. Eu 3+ ions also exhibited biexponential decay in other pyrochlore hosts such as La 2 Hf 2 O 7 , Gd 2 Zr 2 O 7 , and Nd 2 Zr 2 O 7 wherein one of the lifetimes is attributed to A 3+ site occupancy and other to B 4+ site occupancy. , Normally, the short lifetime is attributed to asymmetric environment as f–f transition becomes relaxed, and the long lifetime is mostly attributed to symmetric environment as f–f transition is La Porte forbidden. , The biexponential behavior can also arise due to other reasons such as the presence of defects, energy transfer, and so forth. This phenomenon has been substantiated with theoretical calculations in the next section.…”
Section: Results and Discussionmentioning
confidence: 99%
“…Recent attempts to achieve highly efficient red emission have focused on the doping of materials with rare earth ions. Sm 3+ can achieve highly efficient red‐orange light emission, and high absorbance around 404 nm, which means that it can be effectively excited by an InGaN diode laser, and there are several reports of the optical properties of Sm 3+ in various matrixes, including zirconia phosphors, nanotube arrays, and films . However, to the best of our knowledge, there have been no previous reports of the properties of Sm 3+ doped into yttrium‐stabilized zirconia (YSZ) single crystals.…”
Section: Introductionmentioning
confidence: 99%
“…The first positron lifetime is in close agreement with the positron lifetimes reported on other pyrochlores of the A 2 B 2 O 7 type synthesized at similar temperatures. 40,50,51 In most oxides, the first lifetime component is a combination of positron annihilation in the bulk with few positron traps close by. The dopant Sm 3+ ion is isovalent to La 3+ but smaller in size, while it differs both in size and valency with Ce 4+ .…”
Section: Resultsmentioning
confidence: 99%