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1.
RE 3+ (RE 3+ = Tm 3+, Dy 3+) ion single and co-doped tungsten borate glasses for white light emitting diodes (LEDs) were prepared by melt quenching method. Emission and excitation spectra of the glasses were measured. The color of luminescence can be tuned by changing the composition of glass matrix or the concentrations of Tm 3+ and Dy 3+ ions. White light emission can be achieved from 0.5Dy 3+ single-doped 15WO 3–25La 2O 3–60B 2O 3 and 0.4Tm 3+/1.5Dy 3+ co-doped 50WO 3–25La 2O 3–25B 2O 3 glasses. In addition, energy transfers between Tm 3+ and Dy 3+ were also analyzed. The Dy 3+/Tm 3+ co-doped tungsten borate glasses may be potential candidates for white LED application. 相似文献
2.
A series of color-tunable and white light emitting phosphors BaY 2Si 3O 10:Tm 3+,Dy 3+ were synthesized by a high temperature solid-state reaction, and their phase structure, photoluminescence properties, and energy transfer processes between rare-earth ions were investigated in detail. Upon UV excitation, white light emission depending on dopant concentrations could be achieved by integrating a blue emission band located at 458 nm and an orange one located at 576 nm attributed to Tm 3+ and Dy 3+ ions, respectively. In addition, the energy transfer process between Tm 3+ and Dy 3+ ions was demonstrated to be a resonant type via a dipole–quadrupole mechanism. Preliminary studies showed that the phosphor might be promising as a single-phased white-light-emitting phosphor for UV chip pumped white-light LEDs. 相似文献
3.
Tm 3+ activated germanate-tellurite glasses with good thermal stability and anti-crystallization ability were prepared. Efficient 2 μm fluorescence was observed in the optimal concentration Tm 3+ doped glass and the corresponding radiative properties were investigated. For Tm 3+: 3F 4 → 3H 6 transition, high spontaneous radiative transition probability (260.75 s −1) and large emission cross section (7.66 × 10 −21 cm 2) were obtained from the prepared glass. According to Dexter's and Forster's theory, energy transfer microscopic parameters were computed to elucidate the observed 2 μm emissions in detail. Besides, the effect of hydroxy groups quenching was also quantificationally investigated based on simplified rate equations. Results demonstrate that the optimal concentration Tm 3+ doped germanate-tellurite glass possessing excellent spectroscopic properties might be an attractive candidate for 2 μm laser or amplifier. 相似文献
4.
A white-emitting Ca 9Y(PO 4) 7: Tm 3+, Dy 3+ phosphor has been successfully prepared by conventional high-temperature solid-state reaction. X-ray diffraction (XRD) and fluorescence spectrophotometer were used to characterize the as-synthesized phosphors. The excitation and emission spectra show that all the Tm 3+ and Dy 3+ co-doped Ca 9Y(PO 4) 7 samples can be effectively excited by UV light and then emit blue and yellow light simultaneously. Furthermore, the emission and color coordinate of as-obtained samples pumped by 365 nm are able to be adjusted around white light by varying the doping concentrations of Tm 3+ and Dy 3+. So, the as-fabricated single-composition Ca 9Y(PO 4) 7: Tm 3+, Dy 3+ phosphor will have a promising application in the area of white light emitting diodes. 相似文献
5.
The present paper brings out the results concerning the preparation and optical properties of Sm 3+ and Dy 3+ each ion separately in different concentrations (0.3, 0.5, 1.0 and 1.5 mol.%) and also together doped (x mol.% Dy 3+ + 1.5 mol.% Sm 3+): Li 2O-LiF-B 2O 3-ZnO (where x = 0.5, 1.0 and 1.5 mol.%) glasses by a melt quenching method. Structural and thermal properties have been extensively studied for those glasses by XRD and TG/DTA. The compositional analysis has been carried out from FTIR spectral profile. Optical absorption spectral studies were also carried out. Sm 3+: LBZ glasses have displayed an intense orange emission at 603 nm ( 4G 5/2 → 6H 7/2) with an excitation wavelength at 403 nm and Dy 3+: LBZ glasses have shown two emissions located at 485 nm ( 4F 9/2 → 6H 15/2; blue) and 574 nm ( 4F 9/2 → 6H 13/2; yellow) with an excitation wavelength at 385 nm. Remarkably, it has been identified that the significant increase in the reddish orange emission of Sm 3+ ions and diminished yellow emission pertaining to Dy 3+ ions in the co-doped LBZ glass system under the excitation of 385 nm which relates to Dy 3+ ions. This could be due energy transfer from Dy 3+ to Sm 3+. The non-radiative energy transfer from Dy 3+ to Sm 3+ is explained in terms of their emission spectra, donor lifetime, energy level diagram and energy transfer characteristic factors. These significantly enhanced orange emission exhibited glasses could be suggested as potential optical glasses for orange luminescence photonic devices. 相似文献
6.
Dy 3+ and Tm 3+ co-doped YAl 3(BO 3) 4 (YAB) phosphors were prepared by solid-state reaction method at 1200 °C/3 h. The average crystallite size was determined as 52.09 nm from the X-ray diffraction measurements. Upon 352 and 359 nm near ultra violet excitation, the YAB:Dy 3+–Tm 3+ phosphors exhibit Dy 3+: 4F 9/2 → 6H J ( J = 15/2, 13/2, 11/2) and Tm 3+: 1D 2 → 3F 4 transitions with different luminescence intensity. The photoluminescence emission and decay measurements revealed the energy transfer from Dy 3+ to Tm 3+ ions under 359 nm excitation only. The energy transfer between Dy 3+ and Tm 3+ takes place in Dy 3+–Tm 3+ clusters through exchange interaction mechanism. The Commission International de I’Eclairage chromaticity coordinates of YAB:Tm 3+ phosphor ( λex = 359 nm) were found very close to the European Broadcasting Union and National Television Standard Committee illuminants. The emission color of the studied phosphors could be tuned from blue-to-white as a function of excitation wavelength. The YAB:Dy 3+–Tm 3+ phosphors can be used as potential candidates in display technology. 相似文献
7.
Tm 3+ /Dy 3+ co-doped LiYF 4 single crystals were synthesized by using vertical Bridgman method in sealed Pt crucibles. When excited by a proper UV-light, the crystals show blue emission band centered at 485 nm, which overlaps between the transition of Tm 3+ ( 1G 4 → 3H 6) and Dy 3+ ( 4F 9/2 → 6H 15/2) ions, and yellow band of 573 nm ascribed to Dy 3+ ( 4F 9/2 → 6H 13/2) ions. Both chromaticity coordinates and photoluminescence intensity vary with the excitation wavelengths and the concentration of rare earth dopants. A white light can be achieved from Tm 3+ (0.6 mol%), Dy 3+ (2.25 mol%) co-doped LiYF 4 crystal with chromaticity coordinates of x ≈ 0.2836, y ≈ 0.3229, and color temperature T c = 8419 K by the excitation of a 350 nm light. It indicates that this crystal can be a potential candidate for the UV-light excited white-light emitting diodes. 相似文献
8.
Tm 3+ doped Ga–As–S chalcogenide glass samples were produced using As 2S 3 pure glass as starting materials. Their photoluminescence properties were characterized and strong emission bands were observed at 1.2 μm ( 1H 5 → 3H 6), 1.4 μm ( 3H 4 → 3F 4) and 1.8 μm ( 3F 4 → 3H 6) under excitation wavelengths of 698 nm and 800 nm. The thulium and gallium concentrations were optimized to achieve the highest photoluminescence efficiency. From the optimal composition, a Tm 3+ doped Ga–As–S fiber was drawn and its optical properties were studied. 相似文献
9.
A P 2O 5-CaO-SrO-BaO phosphate glass doped with Tm 3+ and glasses doped with (Tm 3+, Pr 3+) were used for this study. The photo-luminescence behaviors of Tm 3+ and Pr 3+ in phosphate glass were investigated by absorption, excitation and emission spectroscopy. The energy transfer between Tm 3+ and Pr 3+ in phosphate glasses (which exhibit a variety of transfer efficiencies) was studied. The experimental quantum efficiencies of the luminescence of Tm 3+ η0 and (Tm 3+, Pr 3+) doped phosphate glasses were measured to give η/η0 = 0.447, 0.305, and 0.179 for (0.4 mol% Pr 3+, 1.0 mol% Tm 3+), (0.8%Pr 3+, 1.0%Tm 3+) and (1.6 mol% Pr 3+, 1.0 mol% Tm 3+), respectively. In order to verify the nature of the ion coupling in our phosphate glass system, we applied the Inokuti-Hirayama model. The non-radiative energy transfer rate from Tm 3+ to Pr 3+, transfer efficiencies, and the donor-acceptor distance have been calculated and compared with obtained experimental data. As usual, the efficiency and the probability of energy transfer increase with the concentration of the acceptor. 相似文献
10.
Ce 3+ and Dy 3+ activated fluoro-apatite Ca 6La 2Na 2(PO 4) 6F 2 with chemical formulas Ca 6La 2−xLn xNa 2(PO 4) 6F 2 (Ln = Ce 3+, Dy 3+) were prepared by a solid state reaction technique at high temperature. The vacuum-ultraviolet (VUV) and ultraviolet (UV) spectroscopic properties are investigated. The results indicate that Ce 3+ ions show the lowest 5d excitation band at ∼305 nm and a broad emission band centered at ∼345 nm. Dy 3+ ions exhibit intense absorption at VUV and UV range. White-emitting under 172 nm excitation is obtained based on two dominant emissions from Dy 3+ ions centered at 480 and 577 nm. In addition, the energy transfer from Ce 3+ to Dy 3+ in the co-doped samples are observed and discussed. 相似文献
11.
We prepared Er 3+ and Tm 3+ co-doped yttrium oxyfluoride (YOF) powder by combustion synthesis and we observed that under near-infrared ( λ = 980 nm) laser excitation the characteristic green ( 2H 11/2, 4S 3/2 → 4I 15/2) emission of Er 3+ was suppressed by energy transfer (ET) mechanisms between Tm 3+ and Er 3+. The ET process observed in YOF was much more efficient than that observed in standard Y 2O 3 powder prepared under similar conditions. YOF combines the superior mechanical and thermal properties of oxides with low phonon energy of fluorides. Our results show that this material is a serious candidate for use as a red upconversion phosphor. 相似文献
12.
Multicolor and white light emissions have been achieved in Yb 3+, Tm 3+ and Ho 3+ triply doped heavy metal oxide glasses upon laser excitation at 980 nm. The red (660 nm), green (547 nm) and blue (478 nm) up conversion emissions of the rare earth (RE) ions triply doped TeO 2–GeO 2–Bi 2O 3–K 2O glass (TGBK) have been investigated as a function of the RE concentration and excitation power of the 980 nm laser diode. The most appropriate combination of RE in the TGBK glass host (1.6 wt% Yb 2O 3, 0.6 wt% Tm 2O 3 and 0.1 wt% Ho 2O 3) has been determined with the purpose to tune the primary colors (RGB) respective emissions and generate white light emission by varying the pump power. The involved infrared to visible up conversion mechanisms mainly consist in a three-photon blue up conversion of Tm 3+ ions and a two-photon green and red up conversions of Ho 3+ ions. The resulting multicolor emissions have been described according to the CIE-1931 standards. 相似文献
13.
Er 3+/Tm 3+/Yb 3+ tridoped oxyfluoride glass ceramics was synthesized in a general way. Under 980 nm LD pumping, intense red, green and blue upconversion was obtained. And with those primary colors, multicolor luminescence was observed in oxyfluoride glass ceramics with various dopant concentrations. The red and green upconversion is consistent with 4F 9/2 → 4I 15/2 and 2H 11/2, 4S 3/2 → 4I 15/2 transition of Er 3+ respectively. While the blue upconversion originates from 1G 4 → 3H 6 transition of Tm 3+. This is similar to that in Er 3+/Yb 3+ and/or Tm 3+/Yb 3+ codoped glass ceramics. However the upconversion of Tm 3+ is enhanced by the energy transfer between Er 3+ and Tm 3+. 相似文献
14.
Lead fluorophosphate (PbFPDy: P 2O 5 + K 2O + Al 2O 3 + PbF 2 + Na 2O + Dy 2O 3) glasses doped with different Dy 3+ ion concentrations have been prepared and characterized through Raman, absorption, emission and decay rate measurements. Free-ion Hamiltonian model for energy level analysis and Judd–Ofelt theory for spectral intensities have been used to analyze the spectroscopic properties of Dy 3+ ions in lead fluorophosphate glasses. The chromaticity coordinates were calculated from emission spectra and analyzed with Commission International de I’Eclairage color diagram and appear in the white light region under ultraviolet excitation. The decay rates for 4F 9/2 level have been measured and are found to be deviated from exponential to non-exponential nature with increase in Dy 3+ ion concentration. The non-exponential decay rates have been fitted with the Inokuti–Hirayama model for S = 6, which revealed that dipole–dipole mechanism is responsible for the energy transfer processes through Dy 3+–Dy 3+ interaction. 相似文献
15.
The novel Ca 4?x(PO 4) 2O: xDy 3+ and Ca 4?x?y(PO 4) 2O: xDy 3+, yEu 2+ multi-color phosphors were synthesized by traditional solid-state reaction. The crystal structure, particle morphology, photoluminescence properties and energy transfer process were investigated in detail. The X-ray diffraction (XRD) results demonstrate that the products showed pure monoclinic phase of Ca 4(PO 4) 2O when x < 0.1. The scanning electron microscopy (SEM) indicated that the phosphors were grain-like morphologies with diameters of ~ 3.7–7.0 μm. Under excitation of 345 nm, Dy 3+-doped Ca 4(PO 4) 2O phosphors showed multi-color emission bands at 410, 481 and 580 nm originated from oxygen vacancies and Dy 3+. Interestingly, Ca 4(PO 4) 2O: Dy 3+, Eu 2+ phosphors exhibited blue emission band at 481 nm and broad emission band from 530 to 670 nm covering green to red regions. The energy transfer process from Dy 3+ to Eu 2+ was observed for the co-doped samples, and the energy transfer efficiency reached to 60% when Eu 2+ molar concentration was 8%. In particular, warm/cool/day white light with adjustable CCT (2800–6700 K) and high CRI ( Ra > 85) can be obtained by changing the Eu 2+ co-doping contents in Ca 4(PO 4) 2O: Dy 3+, Eu 2+ phosphors. The optimized Ca 3.952(PO 4) 2O: 0.04Dy 3+, 0.008Eu 2+ phosphor can achieve the typical white light with CCT of 4735 K and CRI of 87. 相似文献
16.
A series of novel single-phase white light-emitting Dy3+-doped Ca9Al(PO4)7 nanophosphors was successfully synthesized at 1100 °C via solution combustion route. X-ray diffraction (XRD) and Rietveld refinement analysis of Ca9Dy0.03Al0.97(PO4)7 sample confirmed that this phosphor had a trigonal crystal structure with space group R3c(161). Meanwhile, as-observed from the transmission electron microscopy (TEM) study; particles of Ca9Dy0.03Al0.97(PO4)7 sample were found to have a quadrilateral shape with crystallite sizes around 40–60 nm which were also confirmed by the Debye Scherrer equation. Under near-ultraviolet (NUV) excitation at 350 nm, photoluminescence (PL) emission spectra of nanocrystalline Ca9Al(PO4)7:Dy3+ phosphors showed two peaks at 481 nm and 572 nm corresponding to 4F9/2?→?6H15/2 and 4F9/2?→?6H13/2 transitions, respectively. The optimum concentration was found to be x?=?0.03 mol. The critical energy transfer distance was calculated to be 20 Å and further Huang analysis concluded the exact mechanism, i.e. dipole–dipole interactions responsible for concentration quenching in Ca9DyxAl(1?x)(PO4)7 samples. Furthermore, the Commission Internationale de I’Eclairage (CIE) chromaticity coordinates of Ca9Dy0.03Al0.97(PO4)7 nanophosphor was calculated to be (0.260, 0.297) and this nanophosphor had correlated color temperature (CCT) of 11,332 K which is located in a cool white area. Existing results indicate that Ca9Dy0.03Al0.97(PO4)7 nanophosphor may be considered as a favorable candidate in NUV-based single-phase cool white light-emitting diodes (WLEDs). 相似文献
17.
Y 0.99VO 4:0.01Dy 3+, Y 0.99PO 4:0.01Dy 3+ and Y xVO 4:0.01Dy 3+ phosphors were synthesized by chemical co-precipitation method. All the samples were characterized by X-ray powder diffraction (XRD) and photoluminescence spectroscopy. XRD results show that the samples only have single tetragonal structure and the crystallinity of Y 0.99VO 4:0.01Dy 3+ phosphor is higher than that of Y 0.99PO 4:0.01Dy 3+ phosphor when the heat treatment process is same. Photoluminescence excitation spectra results show that the Y 0.99VO 4:0.01Dy 3+ and Y 0.99PO 4:0.01Dy 3+ phosphors can be efficiently excited by ultraviolet light from 250 nm to 380 nm, the former have a wide Dy 3+–O 2? charge transfer band ranging from 260 nm to 350 nm including a peak at 310 nm, the latter have four peaks at 294 nm, 326 nm, 352 nm and 365 nm. Emission spectra of all the samples exhibit a strong blue emission (483 nm) and another strong yellow emission (574 nm). Moreover, the yellow-to-blue emission intensity ratio and color temperature of emission of Dy 3+ are strongly related to excitation wavelength in Y 0.99PO 4:0.01Dy 3+ phosphor, but it is almost not in Y 0.99VO 4:0.01Dy 3+ phosphor. For Y xVO 4:0.01Dy 3+ ( x = 0.94, 0.97, 0.99, 1.01, 1.03) phosphors, with increasing value of x, the body color of phosphor changes from yellow to white and the strongest peak in excitation spectra shifts a little to shorter wavelength. It is detrimental to luminous intensity when Y 3+ content deviate stoichiometric ratio, but the influence of Y 3+ on the color temperature of emission of YVO 4:Dy 3+ phosphor is slight. 相似文献
18.
Ho 3+ singly doped and Ho 3+/Tm 3+ co-doped hexagonal NaYF 4 powders have been synthesized by a solid-state reaction method. Under excitation of 671 nm diode laser, upconverted blue, green and red emission bands are observed in Ho 3+ singly doped sample. Temporal evolution and excitation power dependent behavior for the green emission are explored, indicating that a photon-avalanche mechanism is responsible for the upconversion processes in Ho 3+ singly doped hexagonal NaYF 4 sample. With the introduction of Tm 3+, the intensities of both blue and green emissions of Ho 3+ are efficiently enhanced, which are attributed to two energy transfer processes from Tm 3+ to Ho 3+, i.e., 3F 4 (Tm 3+) + 5I 8(Ho 3+) → 3H 6 (Tm 3+) + 5I 7(Ho 3+) and 1G 4 (Tm 3+) + 5I 8(Ho 3+) → 3H 6 (Tm 3+) + 5F 3(Ho 3+). The result offers a new sensitization approach to enhance the upconversion efficiency of Ho 3+ under 671 nm excitation. 相似文献
19.
Ultraviolet multiphoton upconversion emissions of Eu 3+ ( 5H3–7, 5G2–6, 5L6 → 7F0) and Gd 3+ ( 6IJ, 6PJ → 8S7/2) are studied in the Eu 3+ (or Gd 3+) doped SiO 2–Al 2O 3–NaF–YF 3 precursor glasses and glass ceramics containing β-YF 3 nanocrystals, under continuous-wavelength 976 nm laser pumping. It is experimentally demonstrated that energy transfer from Yb 3+ to Tm 3+, then further to Eu 3+ or Gd 3+ is responsible for the upconversion process. Compared to those in the precursor glasses, the upconversion emission intensities in the glass ceramics are greatly enhanced, owing to the participation of rare earth ions into the low-phonon-energy environment of β-YF 3 nanocrystals. Hopefully, the studied glass ceramics may find potential applications in the field of ultraviolet solid-state lasers. 相似文献
20.
A series of white-emitting K 2CaP 2O 7:Dy 3+ and K 2CaP 2O 7:Dy 3+, Eu 3+ phosphors were synthesized via a solid-state method, and Eu 3+ was co-doped in K 2CaP 2O 7:Dy 3+ to improve its white light performance. The influences of preparation temperature and Dy 3+/Eu 3+ concentration on the crystal structure and photoluminescence characteristics were investigated. XRD results indicate that K 2CaP 2O 7:Dy 3+ samples prepared above 700 °C matches the standard K 2CaP 2O 7 phase. Under excitation of 349 nm, K 2CaP 2O 7:Dy 3+ phosphor exhibited characteristic emission peaks at 487 nm (blue) and 579 nm (yellow), and white emission was realized through combining these blue and yellow emissions. After co-doping Eu 3+ ions, the co-luminescence of Dy 3+/Eu 3+ with energy transfer between Dy 3+and Eu 3+ were demonstrated. The chromaticity of white light was controlled by changing the ratio of Dy 3+/Eu 3+ concentrations, which lead to a warm white light. Therefore, the results indicate that K 2CaP 2O 7:Dy 3+, Eu 3+ powders have a potential application in w-LEDs as single-component white-emitting phosphor. 相似文献
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