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排序方式: 共有199条查询结果,搜索用时 250 毫秒
11.
热释光油气勘查的机理模型与实验 总被引:1,自引:1,他引:0
多年放射性油气勘查工作研究发现,多数油气藏上方存在放射性异常区.但是,油气藏与其上方放射性异常区是否存在必然联系尚无定论.本文就地表砂土热释光勘查油气藏的机理模型,进行了室内微缩模拟实验,试图证明油气迁移可以引起其上方地层中放射性元素的重新分布与富集.实验中排除了环境辐射差异、地下水活动、地形变化、土质不同等带来的干扰,观察到油气藏上方土层中放射性元素重新分布的迹象.结合前期研究工作可以认为,"油气迁移引起上覆地层中放射性元素重新分布"的假设成立,为研究地表热释光油气勘查方法提供了进一步的理论和事实依据. 相似文献
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《Journal of the European Ceramic Society》2020,40(2):472-479
The oxyfluoride glass and glass-ceramics from the LiF-B2O3-SiO2 system are developed. The stable glass can be produced in the range of 20–40 mol% LiF. The effect of LiF admixture on the thermal stability of the glass as well as the thermoluminescence (TL) properties such as glow curves shape is studied. The results show that the increase of lithium fluoride content in the borosilicate glass causes efficiency enhancement of the thermoluminescence signal. We have clearly stated that the process of controlled crystallization of the oxyfluoride glasses can lead again to increased intensity of the TL process. The glass-ceramics with 40 mol% LiF reveals similar level of TL signal to commercially used doped LiF material and can be considered as active material for alpha and beta radiation detectors. 相似文献
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《中国稀土学报(英文版)》2019,37(11):1132-1136
The Y3(AI,Ga)_5O_(12):Ce~(3+),Cr~(3+),Nd~(3+)(YAGG) nano-phosphors with homogeneous particle-size distribution,low aggregation and average crystalline size of about 65 nm were obtained using a modified Pechini method.Only slight aggregation of the crystallites occurs after post-annealing at 1100℃.The intense Ce~(3+)bands in the excitation spectra of the Ce~(3+),Cr~(3+),Nd~(3+)co-doped materials monitoring the Cr~(3+) emission at 690 nm indicate energy transfer from Ce~(3+) to Cr~(3+).Weak Nd~(3+) lines are observed,as well.In addition,the emission of Nd~(3+)at 1060 nm with excitation of Ce~(3+) and Cr~(3+) confirms the Ce~(3+)/Cr~(3+)to Nd~(3+)energy transfer.The short average luminescence decay times for the Ce~(3+) emission indicate the Ce~(3+)/Cr~(3+)to Nd~(3+)energy transfer.Eventually,the Y_3(AI,Ga)_5O_(12):Ce~(3+),Cr~(3+),Nd~(3+) nano-phosphors exhibit persistent luminescence originating from the 4f~3→4f~3 transitions of Nd~(3+) which matches well to the first biological window to be used in bioimaging applications. 相似文献
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J. Hassinen J. Hls J. Niittykoski T. Laamanen M. Lastusaari M. Malkamki P. Novk 《Optical Materials》2009,31(12):1751-1754
The electronic and defect energy level structure of polycrystalline SrAl2O4:Eu2+,R3+ persistent luminescence materials were studied with thermoluminescence and UV–VUV synchrotron radiation emission and excitation spectroscopy. Theoretical calculations using the density functional theory (DFT) were carried out simultaneously with the experimental work. The experimental band gap energy (Eg) value of 6.6 eV agrees very well with the DFT value of 6.4 eV. The 4f7 → 4f65d1 excitation bands of Eu2+ were found rather similar irrespective of the R3+ co-dopant. The trap level energy distribution depended strongly on the R3+ co-dopant except for the shallowest trap energy above the room temperature remaining the same, however. The different processes in the mechanism of persistent luminescence from SrAl2O4:Eu2+,R3+ was constructed and discussed. 相似文献
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ZnO nanoparticles doped with aluminum (AZO nanoparticles) were investigated using low temperature thermoluminescence (TL) and structural characterization experiments. TL experiments were performed on AZO nanoparticles in the temperature range of 10–300?K. TL curve presented one intensive peak around 123?K and two overlapped peaks to intensive peak around 85 and 150?K for heating rate of 0.1?K/s. Curve fitting and initial rise methods were used to find the activation energies of associated trapping centers. Analyses resulted in the presence of three centers at 0.05, 0.08 and 0.17?eV with peak maximum temperatures (Tm) of 86.2, 121.5 and 147.1?K, respectively. TL experiments were expanded using different heating rates between 0.1?K/s and 0.5?K/s. Behavior of revealed traps was investigated using an experimental technique called as Tm??Tstop method. It was seen that traps are quasi-continuously distributed within the band gap. Structural properties were studied using x-ray diffraction, energy dispersive spectroscopy and scanning electron microscopy experiments. 相似文献
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E.M. Yoshimura E.G. Yukihara 《Nuclear instruments & methods in physics research. Section B, Beam interactions with materials and atoms》2006,250(1-2):337-341
Optically stimulated luminescence (OSL) is increasingly being used as a dosimetric technique in various fields such as medical, environmental and space dosimetry, and sediment and archaeological dating. Nevertheless few compounds are suitable as OSL materials. In this work, a survey was made of various insulators, searching for candidates for new OSL dosimeters. Natural and synthetic crystals and glasses from numerous sources are included. Luminescence was stimulated with blue LEDs (470 nm) and with IR laser (830 nm) provided by an automatic reader. Irradiation was performed with a 90Sr/90Y beta source, and the emitted light was measured with a photomultiplier tube, protected with suitable optical filters. Thermoluminescence (TL) of the samples was also measured, with the same equipment, to evaluate the thermal and optical stability of the defects related to OSL and TL. Among the various investigated materials, Al2O3:Cr, Mg, Fe, MgAl2O4 spinels, Mg2SiO4:Tb, and natural fluorite show potential as OSL dosimeters. Some materials, as barium aluminoborate glasses, although showing intense OSL signals, present a high fading at room temperature. In that situation the OSL signal is related to low temperature TL peaks that also fade at room temperature. None of the investigated materials was specially prepared to be used as an OSL dosimeter, which means that work can be done, mainly in the impurity nature and content, in order to improve OSL signals and to overcome some of the shortcomings that were noticed. 相似文献
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Borates LiSr4(BO3)3 were synthesized by high-temperature solid-state reaction. The thermoluminescence (TL) and some of the dosimetric characteristics of Ce3+-activated LiSr4(BO3)3 were reported. The TL glow curve is composed of only one peak located at about 209 °C between room temperature and 500 °C. The optimum Ce3+ concentration is 1 mol% to obtain the highest TL intensity. The TL kinetic parameters of LiSr4(BO3)3:0.01Ce3+ were studied by the peak shape method. The TL dose response is linear in the protection dose ranging from 1 mGy to 1 Gy. The three-dimensional thermoluminescence emission spectra were also studied, peaking at 441 and 474 nm due to the characteristic transition of Ce3+. 相似文献