2017
DOI: 10.1016/j.jallcom.2017.01.255
|View full text |Cite
|
Sign up to set email alerts
|

Host composition dependent tuneable morphology and luminescent property of the CaXSrYBa1−X−YWO4:RE3+ (RE=Pr, Ho, and Er) phosphors

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

0
7
0

Year Published

2018
2018
2023
2023

Publication Types

Select...
7

Relationship

0
7

Authors

Journals

citations
Cited by 10 publications
(7 citation statements)
references
References 47 publications
0
7
0
Order By: Relevance
“…The broad band located at ∼258 nm can be assigned to host absorption, , which was observed at ∼264 nm for NaLu­(WO 4 ) 2 in this work (Figure S6). The peaks in the 300–500 nm region and located at ∼362, 386, 420, 453, and 487 nm correspond to excitation from the 5 I 8 ground state to the 5 G 2 , 5 G 4 , 5 G 5 , 5 F 1 / 5 G 6 , and 5 F 2 energy levels within the 4f 10 shell of Ho 3+ , as labeled in the figure, ,, with the 5 I 8 → 5 F 1 / 5 G 6 transition at ∼453 nm being the strongest. The Ho 3+ phosphor exhibits strong green emission at ∼545 nm ( 5 F 4 / 5 S 2 → 5 I 8 transition) and weak red emission at ∼650 nm ( 5 F 5 → 5 I 8 transition) under 453 nm excitation.…”
Section: Resultsmentioning
confidence: 93%
“…The broad band located at ∼258 nm can be assigned to host absorption, , which was observed at ∼264 nm for NaLu­(WO 4 ) 2 in this work (Figure S6). The peaks in the 300–500 nm region and located at ∼362, 386, 420, 453, and 487 nm correspond to excitation from the 5 I 8 ground state to the 5 G 2 , 5 G 4 , 5 G 5 , 5 F 1 / 5 G 6 , and 5 F 2 energy levels within the 4f 10 shell of Ho 3+ , as labeled in the figure, ,, with the 5 I 8 → 5 F 1 / 5 G 6 transition at ∼453 nm being the strongest. The Ho 3+ phosphor exhibits strong green emission at ∼545 nm ( 5 F 4 / 5 S 2 → 5 I 8 transition) and weak red emission at ∼650 nm ( 5 F 5 → 5 I 8 transition) under 453 nm excitation.…”
Section: Resultsmentioning
confidence: 93%
“…The luminescent properties of phosphors are affected by the doped rare earth ions, as well as the structure and composition of the substance host [11,12]. Tungstate materials are considered to be effective self-activated fluorescent materials with high-absorption cross-sections [13,14], broadband emissions [15], and high quantum efficiency [16,17].…”
Section: Introduction mentioning
confidence: 99%
“…42,45 Moreover, the emission at 656 nm is attributed to the hypersensitive 3 P 0 → 3 F 2 transition of Pr 3+ (ΔS = 0, ΔJ = 2; S = spin angular momentum, J = total angular momentum), which is a forced electric dipole transition, and strongly dependent on the field environment around Pr 3+ ions. 40 Furthermore, Figure 6A epitomizes the improvement in red emission intensity of CBV: Pr 3+ phosphor with increasing concentration of Pr 3+ ions up to 1.25 mol%. Figure 6B clearly shows that the emission intensity at 608 and 656 nm wavelengths under 473 nm excitation reaches a maximum at 1.25 mol% (optimized concentration) of Pr 3+ ions and decreases contrarily with increasing Pr 3+ concentration owing to concentration quenching phenomenon.…”
Section: Photoluminescence Propertiesmentioning
confidence: 90%
“…The emission spectra reveals various sharp bands located at 533, 547, 583, 608, 620, 656, 680, and 693 nm attributed to 3 P 1 → 3 H 5 , 3 P 0 → 3 H 5 , 3 P 1 → 3 H 6 , 1 D 2 → 3 H 4 , 3 P 0 → 3 H 6 , 3 P 0 → 3 F 2 , 3 P 0 → 3 F 3 , and 1 D 2 → 3 H 5 transitions of Pr 3+ ions, respectively. [37][38][39][40][41][42][43] The emission peak located at 608 nm ( 1 D 2 → 3 H 4 ) dominates among all the peaks present in the emission spectra. In the present case, there is a possibility of inhomogeneous crystal field and low symmetry around Pr 3+ ions, which may be ascribed to minute Ca/Bi disordered ratio in the CBV lattice structure.…”
Section: Photoluminescence Propertiesmentioning
confidence: 99%