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 10 毫秒
1.
Transparent single crystals of AgNiF3 up to 3 mm on an edge have been grown by slow cooling from AgF flux. The crystals are tetragonal, space group D64-p42212, with cell constants a = 5.56 A? and c = 7.86 A?. The material has an optical absorption spectrum typical of divalent nickel in octahedral coordination with fluoride ions. A noncollinear antiferromagnetic transition at 197°K is observed.  相似文献   

2.
Er-doped Lu3Al5O12 (Er:LuAG) single crystalline scintillators with different Er concentrations of 0.1, 0.5, 1, and 3% were grown by the micro-pulling-down (μ-PD) method. The grown crystals were composed of single-phase material, as demonstrated by powder X-ray diffraction (XRD). The radioluminescence spectra measured under 241Am α-ray excitation indicated host emission at approximately 350 nm and Er3+ 4f-4f emissions. According to the pulse height spectra recorded under γ-ray irradiation, the 0.5% Er:LuAG exhibited the highest peak channel among the samples. The γ-ray excited decay time profiles were well fitted by the two-component exponential approximation (0.8 μs and 6-10 μs).  相似文献   

3.
Ce and Eu doped LiSrAlF6 (LiSAF) single crystals for the neutron detection with different dopant concentrations were grown by the micro-pulling-down method (μ-PD). In Ce:LiSAF, intense emission peaks due to Ce3+ 5d-4f transitions were observed at approximately 315 and 335 nm in photo- and α-ray induced radio-luminescence spectra. In case of Eu:LiSAFs, an intense emission peak at 375 nm due to Eu2+ 5d-4f transition was observed in the radio-luminescence spectra. The pulse height spectra and decay time profiles were measured under 252Cf neutron irradiation to examine the neutron response. The Ce 3% and Eu 2% doped LiSAF showed the highest light yield of 2860 ph/n with 19 ns main decay time component and 24,000 ph/n with 1610 ns.  相似文献   

4.
In this work, we report on optical and scintillation properties of a new scintillation material CsGd2Cl7:Ce. Crystals were grown in vacuum sealed ampoules, and the response to gamma rays and thermal neutrons was characterized. The scintillation light yield was ∼38,000 ph/MeV, and the primary decay time was 60 ns under γ-ray excitation. A thermal neutron response resulting from capture by 157Gd and 155Gd and subsequent emission of conversion electrons and X-rays was observed. The crystals exhibited a layered structure with cleavage planes and relatively low hygroscopicity.  相似文献   

5.
为了昨到光折变性能优良的晶体材料,在LiNbO3中掺进CeO2和Eu2O3,生长Ce:LiNbO3和Ce:Eu:LiNbO3单晶体,对晶体进行极化和氧化还原处理,并利用XRD、UV-VIS及二波耦合光路测试了晶体的晶格常数、吸收光谱、指数增益系数和响应时间。结果表明,Ce:Eu:LiNbO3晶体的晶格常数比Ce:LiNbO3晶体小,其吸收边比CeLiNbO3晶体红移更多,指数增益系数比Ce:LiNbO3晶体大,而响应时间比Ce:LiNbO3晶体的要短,Ce:Eu:LiNbO3是优良的光折变晶体材料。  相似文献   

6.
Nd 0.1%, 0.5%, 1% and 3% doped Lu3Al5O12 (Nd:LuAG) single crystals were grown in the nitrogen atmosphere by the micro-pulling down (μ-PD) method. The grown crystals had a single-phase confirmed by powder XRD analysis. In absorption spectra, some weak absorption lines due to Nd3+ 4f-4f transitions were observed and their intensity increased with the increase of Nd concentration. When excited by 241Am α-ray, a broad emission peak due to defects in the host lattice at 320 nm and some sharp lines due to Nd3+ 4f-4f transitions at wavelength longer than 400 nm were observed. The decay time profiles of Nd:LuAG under γ-ray excitation were well approximated by two exponential function of 340-760 ns and 3-5 μs for each sample. By pulse height measurement using 137Cs, Nd 0.5%:LuAG showed the highest light yield of 7600 ± 760 photons/MeV.  相似文献   

7.
Pure, 0.1, 0.5 and 1 mol% Tm-doped YAP single crystalline scintillators were grown by the μ-PD method. The XRD analysis confirmed the lattice constants decrease with the Tm concentration. In the transmittance measurement, the absorption bands due to the Tm3+ 4f-4f transitions were observed at 265, 360, 485, 690 and 800 nm and they were ascribed to the transition from the 3H6 ground state to its 1I6, 1D2, 1G4, 3F3 and 3H4 excited states, respectively. Strong emission peak due to the 1I6-3F4 transition of Tm3+ appeared at 350 nm under X-ray irradiation. The photoluminescence decay time constants related to this transition were evaluated to be from 15.3 to 17.3 μs and the scintillation decay time constants under gamma-ray excitation were estimated to be from 17.5 to 18.8 μs. The Tm 1% doped crystal exhibited the highest light yield of 15, 100 ± 1500 photons/MeV when excited by 137Cs gamma-ray radiation.  相似文献   

8.
在LiNbO3晶体中掺进CeO2和Fe2O3,以Czchralski法生长CeFeLiNbO3晶体,对晶体进行氧化还原处理.测试CeFeLiNbO3晶体的吸收光谱,发现CeFeLiNbO3晶体的吸收边相对LiNbO3晶体发生红移.氧化态的CeFeLiNbO3晶体的吸收边相对还原态的CeFeLiNbO3晶体发生紫移.采用热固定法测试CeFeLiNbO3晶体(氧化,生长,还原)的显影效率.CeFeLiNbO3晶体(还原)的显影效率低于CeFeLiNbO3晶体(氧化)的显影效率.测算并推导出热固定光栅在常温下的寿命.  相似文献   

9.
Sm3+ doped Mg:LiNbO3 and Zn:LiNbO3 are grown by Czochralski method. Optical transmittance and emission spectra are measured and Judd-Ofelt theory is applied to determine phenomenological intensity parameters, oscillator strengths, radiant transition rates, total radiant lifetimes, and branching ratios. The calculations show that Judd-Ofelt parameters with the relation of Ω4 > Ω2 > Ω6 exist, and ΣΩξ (ξ = 2, 4 and 6) in Sm:Zn:LiNbO3 decreases. Fluorescence spectra indicate that visible fluorescence of Sm3+ is made up of 570, 606, 613 and 654 nm emission bands in these crystals under 409 nm excitation.  相似文献   

10.
YVO4 single crystals doped with Ce3+, Er3+ and Yb3+ ions were grown by the Czochralsski technology. The luminescence properties of Er3+/Yb3+:YVO4 single crystals with different concentration of Ce3+ were studied, and the energy transfer mechanism between Er3+, Yb3+ and Ce3+ was discussed based on their energy level properties. The branching ratios of the 4I11/2 → 4I13/2 transition in different samples were calculated. The results indicate that codopants of Ce3+ greatly enhance the population rate of the 4I13/2 level due to the fast resonant energy transfer between Er3+ and Ce3+, i.e., 4I11/2(Er3+) + 2F7/2(Ce3+) → 4I13/2(Er3+) + 2F5/2(Ce3+).  相似文献   

11.
Qiaofeng Han 《Materials Letters》2008,62(14):2050-2052
Orthorhombic Sb2Se3 belts are synthesized via a hydrothermal treatment at 200 °C and pH = 9-10 for 16 h. Transmission electron microscopic (TEM) images show that as-obtained Sb2Se3 belts are with a typical width in the range of 200-400 nm and length up to 20 μm. High-resolution transmission electron microscopic (HRTEM) studies reveal that the Sb2Se3 are oriented in the [001] growth direction. The influences of poly vinyl alcohol (PVA) and the reaction conditions on the formation of belt-like Sb2Se3 microstructures are discussed.  相似文献   

12.
Photoconductivity measurements are applied to the studies of photodynamic processes in LiYF4:Ce3+ and LiLuF4:Ce3+ crystals undergoing ultraviolet irradiation. Photoconductivity spectra were registered by means of microwave technique under irradiation at 220-320 nm at the room temperature. Photoconductivity signal appeared at ∼300 nm and monotonically increased with the shortening of wavelength. Pumping energy dependencies of photoconductivity within 225-305 nm spectral range were registered and revealed the change of the dependence degree from quadratic at longer wavelengths through linear to saturation-like at shorter ones. Numerical simulation based on four-level model of photodynamic processes was performed. Values and spectral distributions of probabilities of different types of photodynamic processes for 225-295 nm were estimated. Ce3+ ions excited-state photoionization cross-section spectra in both investigated materials revealed a band with a peak around 270 nm most probably corresponding to 5d-6s transition of Ce3+. Recombination cross-section in Ce:LiLuF4 appeared to be two orders of magnitude higher than in Ce:LiYF4. A complete energy level diagram of “Ce3+ ion-LiYF4 crystal” system has been proposed.  相似文献   

13.
The Nd-doped and Er-doped LuF3 single crystals were grown by the micro-pulling-down method to study their scintillation properties in the vacuum-ultraviolet (VUV) region. The doubly Nd–Er codoped single crystal was grown to study possibility of scintillation performance improvement by energy transfer from Er3+ to Nd3+ ions. The LiF flux was to avoid phase transition below melting temperature. The 1%Nd-doped sample showed the highest overall scintillation efficiency under X-ray excitation which was 7 times as high as that of the LaF3:Nd 8% standard. The leading Nd3+ 5d–4f emission was situated at 176 nm, while the Er3+ 5d–4f emission for Er-doped samples was observed at 163 nm, which better matches the sensitivity of some VUV-sensitive photodetectors. The optimum Er concentration was determined to be around 1–3 mol%. No Er3+ 5d–4f emission was observed for the doubly Er,Nd-codoped sample due to energy transfer from the Er3+ to Nd3+ ions. Slight improvement of the light yield was observed in the doubly-doped sample with respect to the Nd-only doped one.  相似文献   

14.
Single crystals of defect III–VI semiconductors Ga2Te3 and In2Te3 have been grown by the Bridgman method. Capacitance vs frequency measurements have been carried out from which the low frequency dielectric constants ?5 have been determined to be 10.95 ± 0.26 and 12.3 ± 0.13 respectively. These values are compared with the high-frequency dielectric constants ?60 calculated from the Phillips' model. Dark conductivity and photoconductivity have been studied as a function of annealing upto 210°C, maxinum photosensitivity being obtained for both crystals for Tanneal = 80°C. This behaviour has been related to lattice ordering through x-ray diffraction studies. Measurements of photo conductive gain indicate carrier life-times of 2 × 10?4s and 5 × 10?4s respectively at room-temperature.  相似文献   

15.
The spectroscopic properties of trivalent praseodymium (Pr3+) doped SrLaGa3O7 (SLG) crystals have been investigated at various temperatures. Absorption, emission, excitation and lifetime measurements have been performed and discussed in the framework of the Judd-Ofelt approach. Stimulated emission cross sections for the strongest transitions of Pr3+ ion have been calculated. Stimulated emission has been observed for the first time in Pr3+ doped SLG crystal, we have obtained laser operation at 488 n, at cryogenic temperatures and at 645 nm at room temperature.  相似文献   

16.
为进一步提高骨修复材料的骨诱导性能,引入了BaTiO_3压电涂层。首先,通过等离子喷涂法在Ti基体上制备羟基磷灰石(HA)、Ti-HA和Ti-HA-BaTiO_3这3种生物涂层;然后,采用正交试验设计优化了喷涂工艺参数,用SEM/EDS对涂层的形貌和成分进行了表征,并通过划痕试验测试了涂层与基体的结合强度;最后,进行了细胞培养试验,用CCK-8法对细胞毒性进行了评价,并在SEM下观察了细胞的粘附形态。结果显示:细胞带有伪足,呈梭形和不规则多边形,且粘附在Ti-HA-BaTiO_3复合涂层表面;细胞伸展形态良好,涂层的细胞毒性等级不高于1级。可见,Ti-HA-BaTiO_3复合材料可以作为临床植入材料应用。  相似文献   

17.
18.
Nd3+ doped CaF2 single crystal scintillator has been investigated. We tried to grow 1%, 5%, 10%, 20%, 30% and 40% Nd3+ doped CaF2 single crystals by the simple melt-solidifying method. Powder X-ray diffraction (XRD) patterns were measured to identify the phase of all the samples. The XRD patterns of all the samples were similar to CaF2. Those samples are compared in terms of their X-ray-excited radioluminescence spectra, transmittance, α-ray-excited decay time and light yield. When the X-ray is used for excitation, luminescence is observed in the VUV region. Transmittance of the crystals is more than 70% at wavelengths longer than about 180 nm. In the decay kinetics, the fast components of the samples are distributed in less than 25 ns time range and the slow components of sample are distributed in more than 90 ns. These decay times became shorter with increasing Nd3+ concentration. They are related to the Nd3+ 5d-4f VUV emission. The light yields of samples are distributed in 5-2500 photon/5.5 MeV α-ray and decrease with increasing Nd3+ concentration.  相似文献   

19.
为改善Na0.5Bi0.5TiO3材料的电性能,采用溶胶-凝胶法制备了Na0.5Bi0.5TiO3粉体.通过液相Ce掺杂和气相Ce扩渗两种方法,对Na0.5Bi0.5TiO3粉体进行了改性,采用扫描电子显微镜(SEM)、X射线衍射仪(XRD)、阻抗分析仪和电阻仪对改性前后Na0.5Bi0.5TiO3粉体的组成、结构和电性能的变化进行了研究.结果表明:Ce元素的添加有助于Na0.5Bi0.5TiO3粉体电阻率的降低,而扩渗改性使电阻率的降低更为显著,经600℃扩渗的Na0.5Bi0.5TiO3粉体的电阻率由3.71×106Ω.m降至2.39×101Ω.m;稀土Ce掺杂使Na0.5Bi0.5TiO3的介电常数减小,而Ce扩渗使Na0.5Bi0.5TiO3的介电常数显著增大;Ce掺杂使粒径更加均匀,而随着气相扩渗温度的提高,晶粒粒径逐渐变大;Ce掺杂没有改变Na0.5Bi0.5TiO3的主晶相结构,但Na0.5Bi0.5TiO3粉体经Ce扩渗后,出现了单质Bi及Bi2Ti2O7、Na2Ti9O19、Na2Ti6O13的特征峰.  相似文献   

20.
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