首页 | 本学科首页   官方微博 | 高级检索  
相似文献
 共查询到20条相似文献,搜索用时 453 毫秒
1.
KSrPO4:Tb3+ phosphors were prepared by a solid-state method and their photoluminescence properties were investigated under vacuum ultraviolet excitation. In the excitation spectrum monitoring at 544 nm, the band in the region of 120-162 nm can be attributed to be the overlap of host absorption and charge transfer transition of O2− → Tb3+, and the band ranging from 162 to 300 nm was assigned to the f-d transition of Tb3+. The photoluminescence spectrum shows that the phosphors exhibited a strong green emission around 544 nm corresponding to the 5D4  7F5 transition of Tb3+ under the excitation of 147 nm. Optimal emission intensity was obtained when x = 7% in KSr1-xPO4:xTb3+ and the luminescent chromaticity coordinates were calculated to be (x = 0.317, y = 0.522) for KSr0.93PO4:7%Tb3+.  相似文献   

2.
A series of RE3+ (RE = Ce, Tb, Dy, Tm and Sm) activated Ca10K(PO4)7 were synthesized by conventional state reaction and their photoluminescence properties under vacuum ultraviolet excitation were investigated. The PO43− absorption lies within the range from 125 to 180 nm in all the excitation spectra of Ca10K(PO4)7:RE3+. The first f-d transition of Ce3+ is observed at 316 nm, and the Ce3+ emission is located at about 350 nm. Both the first spin-allowed and spin-forbidden f-d transitions of Tb3+ are situated at 232 and 263 nm, respectively. The emission spectrum of Ca10K(PO4)7:Tb3+ exhibits typical Tb3+ emissions with the predominant peak at 544 nm. The O2−-Dy3+ charge transition band was calculated and identified around 173 nm, the CIE chromaticity coordinates of Dy3+ were calculated to be 0.364 and 0.392. The Ca10K(PO4)7:Tm3+ demonstrates the strongest excitation at about 182 nm assigned to O2−-Tm3+, and gives the predominant emission at 453 nm. The 4G5/2-6H7/2 transition of Sm3+ at 601 nm is the most intensive in the emission spectrum.  相似文献   

3.
LaPO4:Ln3+ (Ln = Eu, Ce, Tb) nanocrystals were successfully synthesized via a facile solvothermal process in the presence of oleic acid. The as-prepared crystals were well characterized by X-ray diffraction (XRD), transmission electron microscopy (TEM), X-ray photoelectron spectra (XPS), Fourier transform infrared spectroscopy (FT-IR), optical spectra as well as the kinetic decay times, respectively. In the synthesis process, oleic acid as a surfactant has played a crucial role in confining the growth and size of the LaPO4:Ln3+ phosphors. All the samples are well crystallized and assigned to the monoclinic monazite-type structure of the LaPO4 phase. The prepared LaPO4:Ln3+ phosphors present a narrow distribution with an average particle size of about 15 nm. Upon excitation by ultraviolet radiation, the LaPO4:Eu3+ phosphors show the characteristic 5D0-7F1-3 emission lines of Eu3+, while the LaPO4:Ce3+,Tb3+ exhibits the characteristic 5D0-7F3-6 emission lines of Tb3+. It is believed that these rare earth ion doped (Eu3+ ion or Ce3+ and Tb3+ ions co-doped) monoclinic monazite-type LaPO4 nanocrystals could find potential application as future advanced optical materials.  相似文献   

4.
The new phosphors Bi2ZnB2O7:Ln3+ (Ln3+ =Eu3+,Dy3+) were synthesized by solid-state reaction technique.The obtained phosphors were investigated by means of X-ray powder diffraction (XRD),photoluminescence excitation and emission spectra with the aim of enhancing the fundamental knowledge about the luminescent properties of Eu3+ and Dy3+ ions in the Bi2ZnB2O7 host lattice.XRD analysis shows that all these compounds are of a single phase of Bi2ZnB2O7.The excitation and emission spectra of Bi2ZnB2O7:Ln3+ (Ln3+ =Eu3+,Dy3+) at room temperature show the typical 4f-4f transitions of Eu3+ and Dy3+,respectively.The hypersensitive transitions of 5D0→7F2 (Eu3+) and 4F9/2→ 6H13/2 (Dy3+) are relatively higher than those of the insensitive transitions in Bi2ZnB2O7.It is conceivable that the Bi2ZnB2O7 structure provides asymmetry sites for activators (Eu3+,Dy3+).The optimum concentrations of Eu3+ and Dy3+ ions in Bi2ZnB2O7 phosphors are both x =0.05.  相似文献   

5.
The core-shell structured LaInO3:Ln3+@SiO2 (Ln3+ = Sm3+, Tb3+) phosphors were realized by coating LaInO3:Ln3+ phosphors on the surface of silica microspheres via a modified Pechini sol-gel process. The phase, structure, morphology, and fluorescent properties of the materials were well characterized by means of X-ray diffraction (XRD), field emission scanning electron microscopy (FE-SEM), transmission electron microscopy (TEM), Fourier transform IR spectroscopy (FT-IR), photoluminescence (PL) spectra, cathodoluminescence (CL) spectra, and the kinetic decays, respectively. The results reveal that the obtained core-shell structured phosphors consist of amorphous silica core and crystalline LaInO3:Ln3+ shell, which keep the uniform spherical morphology of pure silica spheres with narrow size distribution. Upon excitation by ultraviolet (UV) irradiation or electron beam, the phosphors show the characteristic emission lines of Sm3+ (4G5/2-6H5/2,7/2,9/2, orange) in LaInO3:Sm3+@SiO2 and characteristic emissions of Tb3+ (5D4-7F6,5,4,3, green) in LaInO3:Tb3+@SiO2, respectively. This kind of phosphors may have potential applications in field emission displays (FEDs) based on their uniform shape, low-cost synthetic route, and diverse luminescent properties.  相似文献   

6.
High-quality (Gd0.955−xZn0.045)PO4:xTb3+ (0.06≤x≤0.15) green phosphors were synthesized by ultrasonic spray pyrolysis. With an increase of Tb3+ content, the emission intensities caused by the 5D47 F J (J = 3, 4, 5, and 6) and 5D37FJ (J = 4, 5, and 6) transitions of Tb3+ increased and decreased, respectively, allowing a purer green emission. The emission intensity of (Gd0.805Zn0.045)PO4:0.15Tb3+ at 544 nm was 53.0% stronger than that of (Gd0.895Zn0.045)PO4:0.06Tb3+. The emission intensity and the green color purity were remarkably improved by increasing Tb3+ content in (Gd0.955−xZn0.045)PO4:xTb3+.  相似文献   

7.
High-quality Zn-free and added GdPO4:Tb3 green phosphors, i.e., fine size as well as smooth and spherical morphologies, were synthesized by ultrasonic spray pyrolysis. The influence of Zn2+ content and annealing temperature on the photoluminescence properties of the GdPO4:Tb3 phosphors annealed at 800-1100 °C was investigated. The addition of Zn2+ for Gd3+ was highly effective for improving the photoluminescence properties of GdPO4:Tb3. The Zn added GdPO4:Tb3 phosphors with Zn/Gd = 0.045/0.805 showed the strongest emission of the prepared phosphors. The emission intensity at 544 nm for the GdPO4:Tb3 phosphors with Zn/Gd = 0.045/0.805 annealed at 900 °C was 496% stronger than that at 800 °C.  相似文献   

8.
A novel class of orange-red phosphors namely CaLa2ZnO5 (CLZ) doped with Eu3+ ions were prepared by adopting citrate based sol-gel method. Those were thoroughly characterized by means of XRD, SEM, Tg-DTA, photoluminescent (PL) spectral profiles. PL studies reveal that its emission intensity strongly depends on sintering temperature as well as the dopant ion (Eu3+) concentration. Eu3+ ion doped CaLa2ZnO5 phosphor has a strong excitation at 468 nm, which correspond to the popular emission line from a GaN based blue light-emitting diode (LED) chip. The influence of the preparation method on the luminescence property was studied by comparing the emission performance of phosphors prepared by sol-gel and solid-state reaction methods along with a commercial red phosphor Y2O2S:Eu3+. Thus, the intense red emission (5D0 → 7F2) of the Eu3+ doped CLZ phosphors under blue excitation suggests them to be a potential candidate for the production of white light by blue LEDs.  相似文献   

9.
YVO4:Bi3+ phosphors have been prepared by a convenient high-temperature solid-state method. X-ray diffraction (XRD), scanning electron microscopy (SEM) and photoluminescence (PL) technologies are used to study the luminescence properties of YVO4:Bi3+ phosphors. The emission and excitation spectra of Bi3+ in the YVO4 lattice have been investigated at room temperature. The excitation band peaks at 330 nm in a region among 250-400 nm, and the emission spectrum exhibits an intense yellowish-white broad emission centered at about 543 nm covering from 400 nm to 800 nm. The full width at half maximum (FWHM) is about 144 nm. The color coordinates of the as-synthesized YVO4:Bi3+ phosphors are in a range of x = 0.358-0.374, y = 0.482-0.496. The dependence of the luminescence intensity on Bi3+ concentrations and heat treatment condition has also been discussed. In addition, we found that a little amount of flux NH4Cl could enhance the Bi3+ luminescence intensity.  相似文献   

10.
Complex oxides Ln2Mn2/3Re4/3O7 (Ln = Y, Er) and Y2Zn2/3Re4/3O7 with a zirkelite structure and hexagonal unit cells (space group P3121, z = 6) have been obtained. Static and dynamic magnetic susceptibility measurements show that these oxides possess spin-glass behavior at low temperatures. Valence combinations of d-metals in the oxides are Mn2+(Zn2+)–Re5+. It is supposed that the examined specimens Ln2Mn2/3Re4/3O7 (Ln = Y, Er) contain the second magnetic phase of an unknown composition.  相似文献   

11.
Y2O3:Er3+ ultrafine phosphors with a varying Yb3+ ion concentration were prepared by a urea homogeneous precipitation method. The results of XRD show that all the samples are of a pure cubic structure and the average crystallite sizes can be calculated as 45, 34, and 28 nm for Y2O3:Er3+ ultrafine phosphors with Yb3+ ion concentrations of 0, 10%, and 20%, respectively. The lattice constant and cell volume of the ultrafine phosphors decrease with enhancing Yb3+ ion concentration. The upconversion luminescence spectra of all the samples were studied under 980 nm laser excitation. The strong green and red upconversion emission were observed, and attributed to the 2H11/24I15/2, 4S3/24I15/2 and 4F9/24I15/2 transitions of Er3+, respectively. The intensity of red emission increases with increasing Yb3+ ion concentration. The effect of Yb3+ ion concentration on the structures and upconversion luminescence mechanism were discussed.  相似文献   

12.
Phase-pure Ce-/Tb-doped and co-doped lanthanum stannates (La2Sn2O7) nanocrystals were synthesized by a co-precipitation process combined with hydrothermal techniques without any further heat treatment. The crystal structure, particle size, morphologies, and photoluminescence properties of the as-synthesized products were investigated by X-ray powder diffraction (XRD), transmission electron microscopy (TEM), and photoluminescence spectroscopy (PL). The as-prepared samples were single-phase cubic pyrochlore-type nanocrystals with a typical size of 10-20 nm. PL spectra showed a dominating green-emitting line around 544 nm attributing to 5D4-7F5 magnetic dipole transition for Tb3+ doped and Ce3+/Tb3+ co-doped La2Sn2O7 nanocrystals. Meanwhile, the concentration quenching phenomenon was observed in both La2−xTbxSn2O7 and La1.82−xCexTb0.18Sn2O7 nanocrystals. Furthermore, an interesting enhancement of the energy transfer induced green emission was observed in the as-synthesized La1.82−xCexTb0.18Sn2O7 nanocrystals.  相似文献   

13.
Three-dimensional flowerlike YBO3:Tb3+ phosphors have been successfully prepared by an efficient surfactant-free hydrothermal process directly without further sintering treatment. X-ray diffraction (XRD), scanning electron microscopy (SEM), transmission electron microscopy (TEM), energy-dispersive X-ray (EDS) spectrometry, selected area electron diffraction (SAED), photoluminescence (PL) spectra were used to characterize the samples. The as-obtained samples present flowerlike agglomerates composed of nanoflakes with thickness of 20 nm and high crystallinity in spite of the moderate reaction temperature of 180 °C. The reaction mechanism has been considered as a dissolution/precipitation mechanism; the self-assembly evolution process has been proposed on homocentric layer-by-layer growth style. The different luminescent intensity with different molar ratio of Y-Tb [Y:Tb = 8:2; 7:3; 6:4; 5:5; 4:6], YBO3:Tb3+ phosphors exhibit different light (white, red, green) under ultraviolet excitation, which might find potential applications in the fields such as light display systems and optoelectronic devices.  相似文献   

14.
Yb3+ absorption and fluorescent emissions were investigated for NaYbP2O7 diphosphate single crystals. The interpretation of electronic energy level positions has been done by using the comparison of absorption and emission spectra with those of vibronic sideband energy positions from Raman and IR absorption spectroscopies. The Yb3+ energy levels scheme in this host was drawn. The decay time for infrared Yb3+ (5F5/2 excited state) fluorescence was in the range of 1–2 ms. The interest feature is leading to broad emission band at room temperature from 940 nm to 1100 nm, which seems of high interest for ultra-short laser pulse production.  相似文献   

15.
Polycrystalline powder sample of KSr4(BO3)3 was synthesized by high-temperature solid-state reaction. The influence of different rare earth dopants, i.e. Tb3+, Tm3+ and Ce3+, on thermoluminescence (TL) of KSr4(BO3)3 phosphor was discussed. The TL, photoluminescence (PL) and some dosimetric properties of Ce3+-activated KSr4(BO3)3 phosphor were studied. The effect of the concentration of Ce3+ on TL intensity was investigated and the result showed that the optimum Ce3+ concentration was 0.2 mol%. The TL kinetic parameters of KSr4(BO3)3:0.002 Ce3+ phosphor were calculated by computer glow curve deconvolution (CGCD) method. Characteristic emission peaking at about 407 and 383 nm due to the 4f05d1 → 2F(5/2, 7/2) transitions of Ce3+ ion were observed both in PL and three-dimensional (3D) TL spectra. The dose–response of KSr4(BO3)3:0.002 Ce3+ to γ-ray was linear in the range from 1 to 1000 mGy. In addition, the decay of the TL intensity of KSr4(BO3)3:0.002 Ce3+ was also investigated.  相似文献   

16.
The near-stoichiometric LiNbO3 (SLN) single crystals doped Mn2+, Co2+ and Ni2+ in 0.5 mol% concentration in the raw compositions were grown by the Bridgman method under the conditions of taking K2O as flux, a high temperature gradient (90–100 °C/cm) for solid–liquid interface. The XRD, absorption spectra, excitation spectra and emission spectra have been carried out. From the absorption edges of Mn2+, Co2+ and Ni2+-doped SLN crystals, the molar ratio of [Li+]/[Nb5+] are estimated to be about 0.977. The absorption spectra of Mn2+:SLN have shown a broad absorption band centered at 571 nm (6A1g(6S) → 4T1g(4G)), three absorption peaks at 520, 549 and 612 nm (overlapping of the 4T1(F)–4A2(F), 4T1(F)–4T1(P)), and a wide absorption band at 1400 nm (4T1(F) → 4T2(F)) of Co2+:SLN, Ni2+:SLN, and five absorption peaks at 381 nm (3A2g(F) → 3T1g(P)), 733 nm (3A2g(F) → 3T1g(F)), 1280 nm (3A2g(F) → 3T2g(F)), 430 nm (3A2g(F) → 1T2g(D)), and 840 nm (3A2g(F) → 1E(D)) of Ni2+:SLN were observed. A red emission at 612 nm (4T1g(4G) → 6A1g(6S)) for Mn2+:SLN, a red emission at 775 nm (4T1(P) → 4T1(F)) for Co2+:SLN, and a green emission at 577 nm (1T2g(D) → 3A2g(F)) and a red emission at 820 nm (1T2g(D) → 3T2g(F)) for Ni2+:SLN were observed under excited by 416, 520 and 550 nm lights, respectively. The concentration distribution of Mn2+, Co2+and Ni2+ ion in SLN crystals was investigated primarily from the absorption and emission spectra for various parts. The effective distribution coefficient for Mn2+ was less than 1. While, for Co2+ and Ni2+ were more than 1.  相似文献   

17.
This paper reports the photoluminescence (PL) properties of Tb3+ in NaBa4(BO3)3, as well as the time-resolved luminescence properties. The PL excitation spectrum exhibits intense f → f transition absorption; the PL emission spectrum shows the strongest 5D4 → 7F5 emission at 540 nm. The relative intensity of 5D3 emission is much weaker than that of 5D4 emission even in the samples with lower Tb3+ concentration. The 5D3 → 5D4 cross-relaxation produces a marked increase in the 5D3 decay rate with increasing Tb3+ concentrations and introduces a non-exponential component into the initial part of the decay. The dipole-dipole interaction is found to be responsible for the cross-relaxation. The decay curves of 5D4 → 7F5 transition exhibit an initial rise phenomenon. The two exponential fitting indicates that the initial slow rise is attributed to the 5D3 → 5D4 cross-relaxation process.  相似文献   

18.
Mn4+, La3+ and Ho3+ doped MgAl2Si2O8-based phosphors were first synthesized by solid state reaction. They were characterized by thermogravimetry (TG), differential thermal analysis (DTA), X-ray powder diffraction (XRD), photoluminescence (PL) and scanning electron microscopy (SEM). The phosphors were obtained at about 1300 °C. They showed broad red and fuchsia-pink emission bands in the range of 610-715 nm and had a different maximum intensity when activated by UV illumination. Such a fuchsia-pink emission can be attributed to the intrinsic d-d transitions of Mn4+.  相似文献   

19.
The subsolidus phase relations of the SrO–Ta2O5–CuO system were investigated in air. The samples were equilibrated at 900 °C. The ternary oxide Sr3Ta2CuO9 compound is stable under these conditions. This phase presents a solid solution range, its actual composition being Sr3Ta2−xCu1+xO9+δ with 0.0 ≤ x ≤ 0.2. Up to about 5 at.% Cu can be incorporated in the Sr3−xTa1+xO5.5+δ phase. Similarities with the SrO–Nb2O5–CuO system are discussed.  相似文献   

20.
Mn2+ is an excellent luminescent ion with variable color from green, yellow to red in different hosts and has been widely utilized in recent years. The luminescent intensity of Mn2+ in many hosts is so low that the correlative application is restricted. In the present paper, two methods, i.e. employing a charge compensator and introducing a sensitizer, were adopted to enhance the luminescence of Mn2+ in Y3Al5O12 (YAG). By employing Si4+ as a charge compensator, the doping content of Mn2+ (x) in Y3MnxAl5−2xSixO12 can be lifted up to 0.4. Mn2+ in YAG emits orange light in a broad band. The peak wavelength shifts from 586 to 593 nm with the increasing x. The luminescent intensity of Mn2+ reaches its maximum when x = 0.1. Co-doping Tb3+ into Mn2+ doped YAG, the sensitization effect of Tb3+ on Mn2+ was observed clearly. The resonance energy transfer from Tb3+ to Mn2+ occurs because there is a well overlapping between emission spectrum of Tb3+ and excitation spectrum of Mn2+. A reasonable explanation for the sensitization effect of Tb3+ on the luminescence of Mn2+ was brought forward.  相似文献   

设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号