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Lead-free oxyfluoride borate glasses singly doped with Pr3+ and Er3+ were prepared and next investigated using absorption and luminescence spectroscopy. In the studied glass system, barium oxide was substituted by BaF2. Two luminescence bands of Pr3+ located at visible spectral region are observed, which correspond to 3P0–3H4 (blue) and 1D2–3H4 (reddish orange) transitions, respectively. The luminescence bands due to 1D2–3H4 transition of Pr3+ are shifted to shorter wavelengths, when BaO was substituted by BaF2. Near-infrared luminescence spectra of Er3+ ions in lead-free borate glasses modified by BaF2 correspond to 4I13/2–4I15/2 transition. Their spectral linewidths increase with increasing BaF2 concentration. The changes in measured lifetimes of rare earth ions are well correlated with the bonding parameters calculated from the optical absorption spectra. 相似文献
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The absorption and emission of Nd3+:KLa(WO4)2 crystal were investigated. The uniaxial crystal Nd3+:KLa(WO4)2 shows strong polarization dependence. The intensity of the absorption bands in E//c is about four times than that in E//a.
The absorption cross section σa is 22.6 × 10–20 cm2 for E//c. The emission cross section at 1.069 μm is 2.09 × 10–19 cm2. The fluorescence lifetime is 157 μs at 300 K. The relationship of Nd3+ concentrations with fluorescence intensity and lifetime was discussed. The results show the ca 3 at % Nd3+ concentration in Nd3+:KLa(WO4)2 crystal is appropriate.
Electronic Publication 相似文献
4.
The Judd–Ofelt theory has been applied to analyze absorption spectra of Ho3+ ion in HoAl3(BO3)4 measured in spectral range 300–700 nm at room temperature. The Judd–Ofelt spectroscopic parameters have been determined as: Ω2 = 18.87 × 10−20 cm2, Ω4 = 17.04 × 10−20 cm2, Ω6 = 9.21 × 10−20 cm2. These parameters have been used to calculate radiative lifetimes and branching ratios of the luminescence manifolds. Three luminescent bands were found in the spectral range 450–700 nm ascribed to transitions from the 5F5, (5F4, 5S2) and 3K8 states to the ground state 5I8. Experimental intensities of these luminescence transitions were compared with those calculated by using Judd–Ofelt theory and the system of kinetic equations for populations of starting luminescing states. Probabilities of radiativeless transitions were evaluated from this comparison. 相似文献
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《Optical Materials》2005,27(3):475-479
Optical spectroscopy of the green emission of erbium in KGd(WO4)2 (KGW) single crystals codoped with ytterbium ions is investigated. To do this, we firstly grew good-optical-quality KGW single crystals doped with Er3+ and Yb3+ at several dopant concentrations by the Top-seeded-solution-growth slow-cooling method (TSSG). Green photoluminescence of Er3+ in KGW host was studied at room temperature (RT) and low temperature (10 K) by means of Yb3+ sensitization after infrared excitation at 981 nm (10194 cm−1). We calculated the emission and gain cross-sections and compared these with those of other known Er3+-doped laser materials like LiYF4 :Er (YLF:Er) and Y3Al5O12:Er (YAG:Er) at RT. Our study also focused on determining the optimal concentration of ions for generating the most intense green emission. We measured the lifetime of the green emission after infrared pump at several Yb3+ concentrations. From the low-temperature emission experiments, we determined the energy position of the sublevels of the ground state of erbium. 相似文献
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Ma Jingyue Sun Xinran Li Yongji Zhang Xuejian Li Yongtao Liu Huisheng Huang Dexin Zhu Hongguang Qi Haina Mahadevan C. K. 《Journal of Materials Science: Materials in Electronics》2022,33(6):2949-2956
Journal of Materials Science: Materials in Electronics - The NaY(WO4)2:Tm3+,Yb3+ (NYW:Tm3+,Yb3+) and NaY(WO4)2:Tm3+,Er3+,Yb3+ (NYW:Tm3+,Er3+,Yb3+) powders have been synthesized by the... 相似文献
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The spectral parameters of Nd3+ ions in Nd:KLa(WO4)2 crystal have been investigated based on Judd-Ofelt theory. The spectral parameters were obtained: the parameters of oscillator
strengths
are Ω2=3.0887×10–20 cm2, Ω4=1.0375×10–20 cm2, Ω6=1.0422×10–20 cm2, the radiative lifetime is 685 μs, the quantum efficiency is 30.7%, and the fluorescence branch ratios were calculated: β1=0.432, β2=0.475, β3=0.089, β4=0.004.
Electronic Publication 相似文献
8.
《Materials Letters》2004,58(1-2):159-162
Yb3+-doped PbWO4 single crystal was grown using modified vertical Bridgman method. X-ray diffraction (XRD) analysis, optical absorption spectra, X-ray excited luminescence (XEL), fluorescence of 2F5/2→2F7/2 and its lifetime at room temperature were investigated. PWO:Yb3+ shows the broad absorption of Yb3+ (850–1050 nm) and efficient emission (950–1100 nm). Annealing exerts a distinct influence on the PWO:Yb3+ crystal, e.g. disappearance of color and annihilation of the absorption in the region around 450–750 nm, meanwhile the absorption of Yb3+ ions was enhanced by the annealing treatment. A novel luminescence band on the X-ray excited luminescence spectra of PWO:Yb3+ centered at about 500 nm was observed overlapped on that of PWO host. 相似文献
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We report on a comprehensive spectroscopic and laser characterization of monoclinic Yb,Tm:KLu(WO4)2 crystals. Stimulated-emission cross-section spectra corresponding to the 3F4 → 3H6 transition of Tm3+ ions are determined. The radiative lifetime of the 3F4 state of Tm3+ ions is 0.82 ms. The maximum Yb3+ → Tm3+ energy transfer efficiency is 83.9% for 5 at.% Yb – 8 at.% Tm doping. The fractional heat loading for Yb,Tm:KLu(WO4)2 is 0.45 ± 0.05. Using a hemispherical cavity and 5 at.% Yb – 6 at.% Tm doped crystal, a maximum CW power of 227 mW is achieved at 1.983–2.011 μm with a maximum slope efficiency η = 14%. In the microchip laser set-up, the highest slope efficiency is 20% for a 5 at.% Yb– 8 at.% Tm doped crystal with a maximum output power of 201 mW at 1.99–2.007 μm. Operation of Yb,Tm:KLu(WO4)2 as a vibronic laser emitting at 2.081–2.093 μm is also demonstrated. 相似文献
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《Advanced Powder Technology》2020,31(3):1051-1059
Novel up-conversion luminescent SrGd2(WO4)2(MoO4)2: Yb3+/Tm3+/Ho3+ nano-crystals were synthesized by hydrothermal method. The composition ratio of rare earth had been investigated. It indicated that when CYb3+ = 10 mol% and CYb3+/CTm3+/CHo3+ = 10:1.5:2, the emission intensities were the highest. X-ray diffraction (XRD), scanning electron microscope (SEM), transmission electron microscope (TEM) and up-conversion luminescence spectra were used to characterize SrGd2(WO4)2(MoO4)2: Yb3+/Tm3+/Ho3+ nano-crystals and they showed that the sample had high degree of crystallinity, the sample was tetragonal system, and the grain size of the sample was about 56 nm. Three emission peaks, including blue emission peak, green emission peak and red emission peak were observed at 477, 543 and 651 nm corresponding to 1G4 → 3H6 and 1G4 → 3F4 transitions of Tm3+, 5F4 → 5I8 and 5F5 → 5I8 transitions of Ho3+ respectively. All the emission peaks were observed by excitation of 980 nm semiconductor laser. The relationship between up-conversion intensity and excitation power revealed that blue emission at 477 nm was a three-photon absorption process, green emission at 543 nm and red emission at 651 nm was a two-photon absorption process. The quantum yields of the sample were near 3.2%. 相似文献
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YAG晶体中Yb~(3+)对Er~(3+)的敏化作用 总被引:2,自引:0,他引:2
根据能级跃迁速率方程得出Yb,Er:YAG中各能级布居数与Er3+离子浓度的关系.并与单掺Er:YAG中各能级布居数相比较,讨论共掺Yb3+对Er3+的波长为1.64和2.94μm两荧光的影响.结合作者关于红外光激励Yb,Er:YAG能量上转换为可见光工作,提出将Yb,Er:YAG晶体研制成以半导体激光器为激励源的可见光和1.64μm红外光的双波长全固化激光器的设想. 相似文献
12.
通过高温熔融法和热处理制备了含有-γBi2WO6纳米晶的Er3+掺杂透明硼铋酸盐微晶玻璃.根据X射线粉末衍射结果和Scherrer公式计算得到-γBi2WO6晶粒大小约为15 nm.由于部分Er3+离子取代Bi3+进入-γBi2WO6纳米晶相中,使得Er3+离子在1.5μm的有效发射带宽由78 nm增加到85 nm,同时Er3+离子在4I13/2能级的荧光寿命由0.67 ms增加到1.43 ms.此外,与原始玻璃相比,在Er3+掺杂硼铋酸盐微晶玻璃中观察到强烈的绿光上转换发光,其上转换发光机制可以归为双光子过程. 相似文献
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A. N. Georgobiani S. A. Abushov F. A. Kazymova B. G. Tagiev O. B. Tagiev P. Benalloul C. Barthou 《Inorganic Materials》2006,42(11):1188-1192
We have studied the thermo-and photoluminescence of undoped and Er3+-doped EuGa2S4 crystals in the temperature range 77–450 K. In thermoluminescence studies, different heating rates and excitation intensities have been used. The results demonstrate that, with increasing heating rate, the intensity of thermoluminescence peaks grows, and the peaks shift to higher temperatures. EuGa2S4:Er3+ crystals exhibit both Stokes and anti-Stokes luminescence. The mechanisms of these processes are analyzed. 相似文献
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《Optical Materials》2013,35(12):2086-2090
Well oriented KY(WO4)2 single crystal weakly doped simultaneously with Er, Yb and Nd have been investigated using EPR technique. Angular dependencies of the EPR lines clearly confirm C2 symmetry of all: Er3+, Yb3+ and Nd3+ dopants. Basic parameters of the spin Hamiltonian, including Zeeman and hyperfine terms (g and A matrices) as well the spatial orientation between principal axes system and crystallographic axes system were determined. 相似文献
18.
I. T. Bodnar 《Inorganic Materials》2013,49(5):520-524
Data are presented that demonstrate that, when a laser beam polarized at 45° to the vertical (horizontal) is passed through plane-parallel plates cut from a Nd-doped (4%) potassium gadolinium tungstate crystal and placed between crossed polarizers, the intensity and polarization of the transmitted light are periodic functions of the angle of incidence of the light. When scanned in two mutually perpendicular directions, the plates exhibit highly anisotropic transmission. The polarization at the intensity minima and maxima at the analyzer output is not orthogonal, in contrast to uniaxial crystals. 相似文献
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Eu3+, Er3+ and Yb3+ co-doped BaGd2(MoO4)4 two-color emission phosphor was synthesized by the high temperature solid-state method. The structure of the sample was characterized by XRD, and its luminescence properties were investigated in detail. Under the excitation of 395 nm ultraviolet light, the BaGd2(MoO4)4:Eu3+,Er3+,Yb3+ phosphor emitted an intense red light at 595 and 614 nm, which can be attributed to 5D0 → 7F1 and 5D0 → 7F2 transitions of Eu3+, respectively. The phosphor will also show bright green light under 980 nm infrared light excitation. The green emission peaks centred at 529 and 552 nm, were attributed to 4H11/2 → 4I15/2 and 4S3/2 → 4I15/2 transitions of Er3+, respectively. It indicated that the two-color emission can be achieved from the same BaGd2(MoO4)4:Eu3+,Er3+,Yb3+ host system based on the different pumping source, 395 nm UV light and 980 nm infrared light, respectively. The obtained results showed that this kind of phosphor may be potential in the field of multi-color fluorescence imaging and anti-counterfeiting. 相似文献
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M. T. Borowiec V. P. Dyakonov A. Jedrzejczak V. I. Markovich A. A. Pavlyuk H. Szymczak E. E. Zubov M. Załeski 《Journal of Low Temperature Physics》1998,110(5-6):1003-1011
The specific heat C(T) of the monoclinic RbDy(WO
4
)
2
crystal has been studied at very low temperatures 0.2T1.9 K and in magnetic fields 0H0.38 T. The Neel temperature was shown to be equal to TN = 0.818 ± 0.005 K. The experimental value of the effective exchange parameter was obtained to be equal to J/k = – 0.798 K. The C T) dependence below Neel temperature 0.5TN0.99TN
) is well described by 2D Ising model, whereas in the temperature region close above TN
(1.01 TN2TN) it can be described by neither 2D, nor 3D Ising model. The experimental and theoretical H-TN
diagrams for field
H a
are in a reasonable agreement for simple quadratic lattice. 相似文献