Abstract:A series of Dy3+ ion doped Sr2CaWO6 phosphors with double perovskite structure were synthesized by traditional high temperature solid-state method. It was found that there is significant energy transfer between Dy3+ and the host lattice, and the intensities of emission peaks at 449 nm (blue), 499 nm (cyan), 599 nm (orange), 670 nm (red), and 766 nm (infra-red) can be changed by adjusting the concentration of dopant amount of Dy3+ ion in Sr2CaWO6. The correlated color temperature of Dy3+ ion doped Sr2CaWO6 phos… Show more
“…Thus, the ratio is greater than 1 for a centrosymmetric site and less than 1 for a noncentrosymmetric site. [ 36,40,47,48 ] In the current case, the peak related to the MD transition of both Eu 3+ ( 5 D 0 → 7 F 1 ) and Dy 3+ ( 4 F 9/2 → 6 H 15/2 ) ions is stronger than the corresponding ED transition of Eu 3+ ( 5 D 0 → 7 F 2 ) and Dy 3+ ( 4 F 9/2 → 6 H 13/2 ) ions. The ratio of intensity of MD/ED transition is found to be 8.85 for Eu 3+ and 6.09 for Dy 3+ ions, indicating that the occupancy of RE 3+ ions is at the centrosymmetric (i.e., A) site in the cubic DP host lattice.…”
Section: Resultsmentioning
confidence: 59%
“…Thus, the ratio is greater than 1 for a centrosymmetric site and less than 1 for a noncentrosymmetric site. [36,40,47,48] In the current case, the peak related to the MD transition of both Eu 3þ ( 5 D 0 ! 7 F 1 ) and Dy 3þ ( 4 F 9/2 !…”
Section: Pl Studymentioning
confidence: 70%
“…These characteristic peaks are usually attributed to the electronic transition from ground state 6 H 15/2 to respective the excited states 6 P 7/2 , 4 P 3/2 , and 4 F 7/2 of Dy 3þ ion. [47,48] However, these peaks lie in the spectral region of the excitation band of the pure Ba 2 ZnWO 6 host material ( Figure 2). Thus, the narrow characteristic peaks of Dy 3þ ions are found to become broader.…”
Herein, the photoluminescence (PL) and thermoluminescence (TL) properties of rare earth doped cubic double perovskite tungstate Ba2(1−x)(Na,RE)xZnWO6 (RE = Ce3+, Eu3+ and Dy3+) phosphors synthesized by the solid‐state reaction method are presented. The self‐luminescence of pure Ba2ZnWO6 material in the blue‐green region is enhanced by Ce3+ doping with its most effective concentration of 3 mol%. The dominant emission in orange (of Eu3+ at 597 nm) and blue (of Dy3+ at 485 nm) region in the emission spectra of Ba2(1−x)(Na,Eu)xZnWO6 and Ba2(1−x)(Na,Dy)xZnWO6 phosphor, respectively, shows highest intensity for 3 mol% of Eu3+ and 2 mol% of Dy3+ ion in the host lattice. The broad excitation band of Ce3+ and Dy3+ doped phosphor in the near UV region claims its candidature for solid‐state lighting. TL studies are also performed using γ‐radiation. Pure host material shows a simple glow curve while the rare earth ion doped phosphor shows a complex glow curve with enhanced intensity. Phosphor shows the fairly linear response up to 1 kGy radiation. Glow curves are deconvoluted and the trap parameters are calculated by Chen's peak shape method.
“…Thus, the ratio is greater than 1 for a centrosymmetric site and less than 1 for a noncentrosymmetric site. [ 36,40,47,48 ] In the current case, the peak related to the MD transition of both Eu 3+ ( 5 D 0 → 7 F 1 ) and Dy 3+ ( 4 F 9/2 → 6 H 15/2 ) ions is stronger than the corresponding ED transition of Eu 3+ ( 5 D 0 → 7 F 2 ) and Dy 3+ ( 4 F 9/2 → 6 H 13/2 ) ions. The ratio of intensity of MD/ED transition is found to be 8.85 for Eu 3+ and 6.09 for Dy 3+ ions, indicating that the occupancy of RE 3+ ions is at the centrosymmetric (i.e., A) site in the cubic DP host lattice.…”
Section: Resultsmentioning
confidence: 59%
“…Thus, the ratio is greater than 1 for a centrosymmetric site and less than 1 for a noncentrosymmetric site. [36,40,47,48] In the current case, the peak related to the MD transition of both Eu 3þ ( 5 D 0 ! 7 F 1 ) and Dy 3þ ( 4 F 9/2 !…”
Section: Pl Studymentioning
confidence: 70%
“…These characteristic peaks are usually attributed to the electronic transition from ground state 6 H 15/2 to respective the excited states 6 P 7/2 , 4 P 3/2 , and 4 F 7/2 of Dy 3þ ion. [47,48] However, these peaks lie in the spectral region of the excitation band of the pure Ba 2 ZnWO 6 host material ( Figure 2). Thus, the narrow characteristic peaks of Dy 3þ ions are found to become broader.…”
Herein, the photoluminescence (PL) and thermoluminescence (TL) properties of rare earth doped cubic double perovskite tungstate Ba2(1−x)(Na,RE)xZnWO6 (RE = Ce3+, Eu3+ and Dy3+) phosphors synthesized by the solid‐state reaction method are presented. The self‐luminescence of pure Ba2ZnWO6 material in the blue‐green region is enhanced by Ce3+ doping with its most effective concentration of 3 mol%. The dominant emission in orange (of Eu3+ at 597 nm) and blue (of Dy3+ at 485 nm) region in the emission spectra of Ba2(1−x)(Na,Eu)xZnWO6 and Ba2(1−x)(Na,Dy)xZnWO6 phosphor, respectively, shows highest intensity for 3 mol% of Eu3+ and 2 mol% of Dy3+ ion in the host lattice. The broad excitation band of Ce3+ and Dy3+ doped phosphor in the near UV region claims its candidature for solid‐state lighting. TL studies are also performed using γ‐radiation. Pure host material shows a simple glow curve while the rare earth ion doped phosphor shows a complex glow curve with enhanced intensity. Phosphor shows the fairly linear response up to 1 kGy radiation. Glow curves are deconvoluted and the trap parameters are calculated by Chen's peak shape method.
“…Recently, Mn 4+ -activated Sr 2 ZnWO 6 and LiLaMgWO 6 were investigated as red-far-red phosphors for plant cultivation LEDs. , However, actually, their poor luminescence thermal stability in them makes inappropriate for practical application, which also often takes place in other kinds of Mn 4+ -activated double-perovskite phosphors such as (Ba 1– x Sr x ) 2 YSbO 6 :Mn 4+ , Ca 2 GdSbO 6 :Mn 4+ , Sr 2 YNbO 6 :Mn 4+ , LiLa 2 TaO 6 :Mn 4+ , Ca 2 LaNbO 6 :Mn 4+ , etc., − since the working temperature of pc-LEDs can reach above 423 K. Consequently, it is urgent and significant to improve the thermal luminescence quenching performance for current materials or search for novel red-far-red luminescence materials with extraordinary luminescence thermal stability. Recently, Sr 2 CaWO 6 , a double-perovskite compound, was used as a matrix for rare earth (Re 3+ = Dy 3+ , Sm 3+ , Eu 3+ ) ions doping and their luminescence properties were investigated in detail. − As mentioned above, there are suitable WO 6 octahedrons in this double-perovskite compound for Mn 4+ incorporation. Unfortunately, we found that the luminescence of Sr 2 CaWO 6 :Mn 4+ is too feeble to be intuitively observable under a 302/365 nm UV lamp irradiation.…”
In this work, we adopt a facile rare earth ions Ln 3+ (Ln = La, Gd, Y, Lu) substitution strategy to achieve the efficient red luminescence Sr 2 Ca 1−δ Ln δ WO 6 :Mn 4+ (δ = 0.10), which extremely improves the luminescence properties of luminescence-ignorable Sr 2 CaWO 6 :Mn 4+ . It is demonstrated that the substitution of Ln 3+ for Ca 2+ can stabilize the Mn in tetravalent state, which would like to occupy W 6+ site and generate the luminescence. It is also found that the emission profile of original Sr 2 CaWO 6 :Mn 4+ changes manifestly after different Ln 3+ ions substitution, which is mainly attributed to the synergistic effect of lattice distortion, Mn 4+ transition 2 E g → 4 A 2g and lattice vibration. Most fascinatingly, the Sr 2 Ca 0.9 Ln 0.1 WO 6 :0.005Mn 4+ (SC 0.9 Ln 0.1 WO:0.005Mn 4+ , Ln = La, Gd) show extraordinary luminescence thermal stability, whose integrated emission intensity still maintains about 95% (Gd, 96.8%; La, 94.8%) at 478 K of its original value at room temperature (298 K), much better than those in most reported Mn 4+ -activated oxide phosphors so far. It is confirmed that the traps may play an important role for this phenomenon. Best of all, this work gives us a facile strategy to achieve efficient Mn 4+ -activated red-emitting materials with extraordinary luminescence thermal stabilities derived from luminescence-ignorable ones.
“…17–19 According to the literature, some Dy 3+ activated materials show weak red emission around 670 nm due to the 4 F 9/2 → 6 H 13/2 transition. 20 Due to the absence or a weak red color emission, Dy 3+ activated materials show a very poor color rendering index. To solve this problem, Eu 3+ ions can be co-doped in the host material in the presence of the Dy 3+ ion.…”
In the present investigation, different concentrations of Dy3+, Eu3+ doped and co-doped La(PO4) phosphors were synthesized via the solid-state synthesis route. Further, their structural, morphological, vibrational features, thermal stability, spectroscopic...
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