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Y2O3纳米晶中两种格位的Eu3+之间的能量传递 总被引:2,自引:2,他引:0
讨论了Eu^3 :Y2O3纳米晶在低温下的发光性质。比较了不同颗粒尺寸的Y2O3纳米晶中Eu^3 离子的发射光谱,根据不同温度下的激发谱,分析了处于Y2O3纳米晶中C2和C3i两种格位的激发峰强度随温度的变化,选择激发了不同格位的孤立的Eu^3 离子和处于相邻格位(C3i-C2)的Eu^3 离子对,结果表明,相邻Eu^3 离子对的能量传递速率比孤立的Eu离子之间的能量传递速率快,分析了纳米Eu^3 :Y2O3中猝灭浓度提高的原因。 相似文献
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Y2O2S:Eu3+,Mg2+,Ti4+红色材料的制备和长余辉性能 总被引:17,自引:9,他引:8
用高温固相法制备了Y2O2S:Eu^3 ,Mg^2 ,Ti^4 红色长余辉材料,余辉时间达到1h以上,X射线衍射测量表明材料的晶体结构为Y2O2S。发射光谱对应了Eu^3 离子^5DJ(J=0,1,2,3)→^7FJ(J=0,1,2,3,4))的特征发射;激发光谱主峰位于345nm,另外在260,396,468,540nm等处也存在激发峰。对比测量了Y2O2S:Eu^3 ,Mg^2 ,Ti^4 和Y2O2S:Eu^3 的热释发光曲线,Y2O2S:Eu^3 的热释发光曲线可以拟合成3个热释发光峰的叠加:237,226,301K;而Y2O2S:Eu^3 ,Mg^2 ,Ti^4 的热释发光曲线可以拟合成5个热释发光峰的叠加:149,215,262,287,334K,并计算了相应的陷阱能级。Ti^4 是引起较深陷阱能级的主要原因,Mg^2 起电荷补偿的作用。 相似文献
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纳米晶Gd2O3:Eu^3+的制备及发光性能 总被引:2,自引:3,他引:2
采用低温燃烧合成法制备了Gd2O3:Eu^3+纳米晶。用X射线衍射仪(XRD)、高分辨透射电子显微镜(HRTEM)和荧光光谱仪分别对样品的结构、形貌和发光性能进行了研究。结果表明,改变甘氨酸与稀土离子的比例(G/M)、退火温度可以制备出不同结构和晶粒尺寸的Gd2O3:Eu^3+纳米晶。在退火温度为800℃,G/M等于0.83和1.0时,均得到了纯立方相的Gd2O3:Eu^3+纳米晶,随着G/M的增加,Gd2O3:Eu^3+从立方相逐渐向单斜相转变。粉末的晶粒尺寸随着退火温度的增高而增大,晶粒尺寸在10-30nm之间。立方相的Gd2O3:Eu^3+纳米晶主发射峰位置在612nm(^5D^0→^7F2跃迁),激发光谱中电荷迁移态发生了红移。 相似文献
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为进一步提高Y2O2S:Eu^3+的发光性能,采用改善主要原材料Y2O3结晶性的方法,使Y2O2S:Eu^3+红色荧光粉在20kV和25kV下发光强度分别增强5%和10%,且不影响色度、粒度、粉体分散性等主要考核指标。提高了粉体的耐电压特性(发射强度与激发电压间的关系特性)。讨论和分析了发射强度增强、电压特性改善的原因:主要原材料Y2O3的结晶性的改善,使得合成的Y2O2S:Eu^3+具有更好的晶体质量,Eu^3+离子品场环境得到进一步改善,从而减弱了无辐射过程及因晶格畸变所造成的能量损失,发光效率得到增强,电压特性得刮改善。文验表明,获取高质量多晶Y2O3的最佳分解温度为1400℃左右。 相似文献
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Summary We report the measurements of the3
D(3s4d)-3
P(3s3p)3
D(3s5d)-3
P(3s3p), and3
P(3p
2)-3
P(3s3p) transition frequency of MgI, the fine-structure separation and isotope shift between24Mg and26Mg. The measurements have been performed in a metastable atomic beam; a good agreement is found for data already existing
in the literature. The accuracy of the measurements reported in this paper is mainly limited by the Doppler broadening of
theI
2 transitions used as a reference and by the precision in the knowledge of the related wavelengths. 相似文献
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The systematic application of band contour techniques to account for most of the observed features of the ir spectra of s-triazine and s-triazine-d3 have been made as well as a critique as to the limitations of such methods. The experimental and computer methods used to study the gas phase infrared band contours of s-triazine and s-triazine-d3 are out-lined. Contours of the five E′ fundamentals of s-triazine have been recorded under moderate resolution and analyzed to give the Coriolis constants , i = 6–10. The effects of l-resonance are very apparent for ν8 and ν9, in the form of holes in the Q branches of these bands. Under the highest resolution available, ν6 and ν10 also show l-resonance effects. Values of the l-doubling constants were obtained for these four fundamentals. One of the parallel A2″ fundamentals of C3H3N3 (ν12) has also been studied. It lies close to ν10(E′) and an A × E type of second-order Coriolis resonance may be the cause of the intensity enhancement observed in the inner wings of the ν12 and ν10 bands. Hot bands of the type (νi + nν14 ? nν14) have been observed in the contours of ν8, ν10, and ν12. This is felt to be responsible for the large difference between our observed zeta sum (?1.30) and the theoretical sum (?1.00).The gas phase infrared band contours of the five E′ and 2A2″ fundamentals of C3N3D3 have also been recorded under moderate resolution. From P-R separations and by computer simulation of the contours, values of the Coriolis constants have been obtained for the E′ modes. The effects of l-resonance have been observed for ν8(E′) and ν10(E′) and values of the l-doubling constants have been estimated. An extensive series of hot bands of the type (ν12 + nν14 ? nν14) has been observed in the contour of the ν12 (A2″) fundamental. The mass effect on the Coriolis constants has been discussed.Infrared band contours of the overtone 2ν7 and seven degenerate E′ combination bands of C3N3H3 have been recorded under moderate resolution. Analysis of these contours using the P-R separation method and computer simulation of the contours has given values of for these bands. Fermi resonance between 2ν7 and ν6 has been analyzed. The importance of considering both the observed contour as well as the observed frequency when assigning higher tone bands is illustrated. 相似文献
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P. A. Markovin V. V. Lemanov M. E. Guzhva P. P. Syrnikov T. A. Shaplygina 《Physics of the Solid State》2014,56(5):989-995
The temperature dependences of the dielectric constant and dielectric hysteresis loops in ceramic samples of (1 ? x)SrTiO3?x KNbO3 and (1 ? x)SrTiO3?x KTaO3 (0 ≤ x ≤ 0.3) solid solutions prepared using different heat treatments have been investigated. Phase diagrams of the studied solid solutions have been constructed in the T-x coordinates. It has been shown that, after quenching of samples (spontaneous cooling at room temperature after long-term heating at the sintering temperature of the ceramic samples), the temperature of the induced phase transition increases because of the weakening of random electric fields associated with nonisovalent impurities due to their “frozen” nonequilibrium redistribution. For small concentrations x, strong dielectric relaxation is observed in the temperature range of 150–250 K. A model of relaxing centers, which is based on the local charge compensation of heterovalent impurities, has been proposed. 相似文献
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The infrared spectra of ammonia-borane, BH3NH3, and two of its deuterated isotropic species, BD3ND3 and BH3ND3, isolated in argon matrix at liquid hydrogen temperature have been measured. Well resolved bands for these three isotopic species have been observed for all the fundamentals. A complete frequency assignment based on C3v molecular symmetry has been made. A set of force constants have been calculated from the data for the two isotopes BH3NH3 and BD3ND3 using a valence force field. The agreement between experiment and frequencies calculated from these force constants for the mixed isotopic species, BH3ND3, substantiates the present assignment. 相似文献
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Knorr K. Loidl A. Stühn B. Buevoz J. L. 《Zeitschrift für Physik B Condensed Matter》1981,41(4):315-320
Neutron diffraction experiments have been carried out on the magnetically ordered phases of ErPb3, HoPb3, ErTl3 and HoTl3. The magnetic moments were found to be sinusoidally modulated with a propagation vector of (0, 0.2, 0.5) for the Pb-compounds and (0.38, 0.38, 0.16) for the Tl-compounds.Work supported by the Bundesministerium für Forschung und Technologie 相似文献
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Improvement of Photoluminescence of Perovskite CH_3NH_3Pb I_3 by Adding Additional CH_3NH_3I during Grinding 下载免费PDF全文
《中国物理快报》2021,(8)
The organic-inorganic hybrid perovskite CH_3NH_3PbI_3 has been a good candidate for many optoelectronic applications such as light-emitting diodes due to its unique properties.Optimizing the optical properties of the CH_3NH_3PbI_3 material to improve the device performance is a hot topic.Herein,a new strategy is proposed to enhance the light emission of CH_3NH_3PbI_3 phosphor effectively.By adding the reactant CH_3NH_3I powder in an appropriate proportion and simply grinding,the emission intensity of CH_3NH_3PbI_3 is greatly improved.The advantages of the proposed method are swiftness,simplicity and reproducibility,and no requirement for a complex organic ligand.The mechanism of this phenomenon is revealed by x-ray diffraction,scanning electron microscopy,energy dispersive spectroscopy,photoluminescence,and temperature-dependent photoluminescence.This study offers a unique insight for optimizing the optical properties of halide perovskite materials. 相似文献
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Abstract Spectra of polycrystalline samples of NH3BF3 and ND3BF3 at 300 K and 98 K have been recorded in the frequency range 20-400 cm?1. Isotopic frequency ratios are used to interpret the observed features in terms of the known molecular and crystal structures. 相似文献
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Sulai IA Wu Q Bishof M Drake GW Lu ZT Mueller P Santra R 《Physical review letters》2008,101(17):173001
Two anomalously weak transitions within the 2(3)S_(1)--3(3)P_(J) manifolds in 3He have been identified. Their transition strengths are measured to be 1000 times weaker than that of the strongest transition in the same group. This dramatic suppression of transition strengths is due to the dominance of the hyperfine interaction over the fine-structure interaction. An alternative selection rule based on IS coupling (where the nuclear spin is first coupled to the total electron spin) is proposed. This provides qualitative understanding of the transition strengths. It is shown that the small deviations from the IS coupling model are fully accounted for by an exact diagonalization of the strongly interacting states. 相似文献