共查询到17条相似文献,搜索用时 718 毫秒
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单能X射线光源是由X射线光机、双晶单色器、标准探测器以及准直系统组成。X射线光机产生的连续X射线,通过与双晶单色器发生布拉格衍射完成单色化,调节不同的特定布拉格角度得到能量范围30~160keV的单能X射线。为了研究标定装置的能量展宽,需要对该装置产生的单能X射线的能量分辨率进行研究。结果表明Si(220)晶体产生的单能X射线的能量分辨率为0.91%@30keV和2.3%@70.6keV,Si(551)晶体为1.97%@80.1keV和3.45%@142.6keV。使用这套装置对溴化镧晶体探测器的能量响应进行校准验证,实验发现该装置的能量分辨率良好,可以应用在多种类型探测器的标定实验、X射线质量衰减系数测量以及多层膜反射率测量等领域。 相似文献
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随着国内X光机数量的迅速增多,简易有效的X光机半值层(HVL)质量检测方法也越来越重要。使用Penelope软件模拟N80(65keV)、N100(83 keV)、N150(118keV)、N200(164keV)重过滤窄谱辐照场中氟化锂热释光(LiF(Mg,Cu,P))剂量计在不同铜过滤片厚度下的能量沉积,分析计算得到X光机HVL; 通过实验测量LiF在N100(83keV)3m处窄谱标准辐照场的X光机HVL,对模拟程序进行了验证。对模拟结果与标准实验室电离室测量结果进行比较表明:对于低能N80(65keV)、N100(83keV)辐照场,LiF剂量计测量X射线半值层的方法具有可行性;N150(118keV)、N200(164keV)辐照场中模拟结果与实验室给出电离法测量得到的半值层值相对误差较大,不建议直接使用LiF测量半值层。 相似文献
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CdTe探测器对单能平行光子源的绝对测量之前,需要进行效率刻度。利用MCNP5蒙特卡罗模拟程序建立CdTe探测器物理模型,模拟计算了10~260keV能量段能点的本征探测效率,在10~60keV能量段探测效率高于75%。用单能X射线装置和HPGe探测器对CdTe探测器本征探测效率进行了实验刻度。结果表明,在10~100keV能量范围内CdTe探测器的模拟效率与实验效率趋势一致,最大误差不超过5.6%。因为Te元素在27keV和32keV处会产生逃逸峰,导致探测效率在这2个能量处有明显下降趋势。用241Am和133Ba放射源对CdTe探测器进行效率刻度验证,在能量为59.54keV和81keV放射源标定的探测效率与单能X射线辐射装置测量值相符。 相似文献
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为了研究不同限束光阑准直器对测量结果的影响,使用MCNP5蒙卡模拟软件建立带准直器的高纯锗探测器模型。通过模拟分析准直器各项参数对高纯锗探测器测量X射线能谱的影响,确立了准直器的最佳尺寸,为实验室使用高纯锗探测器测量X射线能谱提供一定的参考依据。计算了透射等效孔径(TEA)准直器指标,分析了高纯锗探测器测量X射线得到的探测效率。结果表明:对于能量小于80keV的低能量段X射线能谱测量,选择孔径小、屏蔽厚的准直器;对于80keV以上中高能量段的X射线应选择较大孔径的准直器,以避免由于从铅准直器中产生小角散射线和铅的特征线而影响X射线能谱的质量。 相似文献
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带支撑结构的大高宽比硬X射线波带片制作 总被引:3,自引:2,他引:1
对利用X射线光刻制作大高宽比硬X射线波带片的设计和制作工艺进行了研究.采用电子束光刻制作X射线光刻掩模,并利用X射线光刻制作最终的硬X射线波带片.采用对光刻胶结构加入支撑点的方法,大大提高了X射线光刻制作硬X射线波带片的高宽比.对所加入支撑点的布置策略进行了优化,使得支撑点所占的面积比例减小.所制作的波带片最外环宽度为200 nm,厚度为2.8μm,具有优良的结构质量,预期可用于10 keV到25 keV波段,并具有优于250 nm的成像分辨率. 相似文献
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为建立高注量率同步辐射X射线计量领域相关的国家标准,对同步辐射X射线能量标定方法进行研究。在北京同步辐射装置上选择6、10和20keV三个能量点进行实验,得到的传递探测器校准因子与辐射能量的关系曲线近似直线,变化趋势呈线性递减;在20keV能量点,不同直径光阑条件下进行的标定实验验证了传递探测器的校准因子与光源照射到基准电离室与传递探测器的光子通量有关。在上海光源上进行10~70keV能量标定实验,得到传递探测器的校准因子拟合曲线;10~20keV能量段的变化趋势与在北京同步辐射装置得到的校准因子变化趋势一致,30~70keV能量段的校准因子随着能量的增加而平稳缓慢增大。对各个能量点标定产生的A类不确定度进行评定,为后续建立国家计量标准同步辐射X射线空气比释动能量值传递体系提供了技术数据。 相似文献
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《中国测试》2020,(4)
线性衰减系数是放射性体源测量中进行自吸收修正的重要参数。由于能量不同,无法用人工核素点源的透射实验获得对应于天然核素发射γ射线能量的线性衰减系数值。该文提出一种新的拟合公式和拟合方法,以便由人工核素点源透射实验获得的γ射线线性衰减系数求出被测样品在天然核素γ射线能量点的线性衰减系数。对选用的5种被测物质,分别用线性衰减系数的参考值和实测值进行拟合之后的计算结果显示,在γ射线能量为60~2 600 keV的范围内,该文提出的拟合方法计算出来的线性衰减系数的最大误差分别小于4%和10%。利用该文介绍的拟合方法,可以得到被测样品在指定能量范围内比较准确的线性衰减系数值。 相似文献
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Some building materials, regularly used in Turkey, such as sand, cement, gas concrete (lightweight, aerated concrete), tile and brick, have been investigated in terms of mass attenuation coefficient (μ/ρ), effective atomic, numbers (Z(eff)), effective electron densities (N(e)) and photon interaction cross section (σ(a)) at 14 different energies from 81- to 1332-keV gamma-ray energies. The gamma rays were detected by using gamma-ray spectroscopy, a High Purity Germanium (HPGe) detector. The elemental compositions of samples were analysed using an energy dispersive X-ray fluorescence spectrometer. Mass attenuation coefficients of these samples have been compared with tabulations based upon the results of WinXcom. The theoretical mass attenuation coefficients were estimated using the mixture rule and the experimental values of investigated parameters were compared with the calculated values. The agreement of measured values of mass attenuation coefficient, effective atomic numbers, effective electron densities and photon interaction cross section with the theory has been found to be quite satisfactory. 相似文献
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In connection with the design of a hard-x-ray telescope for the Constellation X-Ray Observatory we measured the reflectivity of an iridium-coated zerodur substrate as a function of angle at 55, 60, 70, and 80 keV at the National Synchrotron Light Source of Brookhaven National Laboratory. The optical constants were derived from the reflectivity data. The real component of the index of refraction is in excellent agreement with theoretical values at all four energies. However, the imaginary component, which is related to the mass attenuation coefficient, is 50% to 70% larger at 55, 60, and 70 keV than theoretical values. 相似文献
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S. Okada D. A. Bennett W. B. Doriese J. W. Fowler K. D. Irwin S. Ishimoto M. Sato D. R. Schmidt D. S. Swetz H. Tatsuno J. N. Ullom S. Yamada 《Journal of Low Temperature Physics》2014,176(5-6):1015-1021
We are preparing for an ultra-high resolution X-ray spectroscopy of kaonic atoms using an X-ray spectrometer based on an array of superconducting transition-edge-sensor microcalorimeters developed by NIST. The instrument has excellent energy resolutions of 2–3 eV (FWHM) at 6 keV and a large collecting area of about 20 mm \(^2\) . This will open new door to investigate kaon-nucleus strong interaction and provide new accurate charged-kaon mass value. 相似文献
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M. I. Sayyed Y. Elmahroug B. O. Elbashir Shams A. M. Issa 《Journal of Materials Science: Materials in Electronics》2017,28(5):4064-4074
In the present work, the gamma ray shielding properties of zinc oxide soda lime silica, (ZnO)x(SLS)1?x glasses with 0 ≥ x ≥ 50 wt% have been investigated. By using WinXCom computer software, the mass attenuation coefficient (µ/ρ) and half value layer (HVL) for total photon interaction in the energy range of 1 keV–100 GeV were calculated. Furthermore and by Geometric Progression method exposure buildup factor values were calculated for incident photon energy 0.015–15 MeV up to penetration depths of 40 mfp (mean free path). The addition of zinc oxide (ZnO) into soda lime silica (SLS) glass resulted in an increase the mass attenuation coefficient and decreases both the half value layer and exposure buildup factor. The obtained results of the selected glass series have been compared, in terms of mass attenuation coefficient, half value layer and exposure buildup factor with some common shielding materials. The shielding effectiveness of the selected glasses is found comparable to that of common ones; which indicates that the SLS glasses with suitable ZnO content may be developed as gamma ray shielding materials. 相似文献
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S. Ammiraju R. Madhusudhan K. Narender K. G. K. Rao N. G. Krishna 《High Temperature》2014,52(5):640-653
The temperature dependence of linear attenuation coefficient, density and thermal expansion of rubidium halides (RbCl, RbBr and RbI) and lithium halides (LiCl, LiBr and LiF) has been studied by γ-ray attenuation technique. The γ-ray attenuation studies have been carried out using a γ-ray densitometer. The mass attenuation coefficients (μ m ) of rubidium and lithium halides have been determined using γ-beam of different energies viz. (0.0595, 0.662, 1.173 and 1.332 MeV) respectively. The variation of density and coefficients of temperature dependence of density have been measured using Cs (0.662 MeV) source. The values of density at different temperatures have been used to estimate the values of linear attenuation coefficients (μ l ) of the alkali halides studied in the present work for other γ-energies. The variation of thermal expansion of alkali halides studied in the present work has been compared with the results obtained from other methods. The variation in these thermophysical properties have been represented by linear equations. Volume thermal expansion coefficients and mass attenuation coefficients (μ m ) of these compounds for the different energies have been reported and compared with data calculated by empirical and experimental method. 相似文献
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Almeida CD Coutinho CM Dantas BM Peixoto JE Koch HA 《Radiation protection dosimetry》2012,151(1):196-198
Breast phantoms produced with tissue-equivalent materials are used in an attempt to simulate glandular and adipose tissues, in terms of X-ray attenuation and density. In this work, a set of breast tissue-equivalent phantoms (BTE phantoms) with semicircular shapes of different thicknesses and compositions were produced. Such phantoms may be used in the measurement of the incident air kerma (K(i)) and the mean glandular dose (D(G)) delivered to patients undergoing mammography. To characterise the materials used to produce the phantoms, a series of 17-keV X-ray attenuation coefficient measurements were performed. The carbon-nitrogen-hydrogen elemental composition and the densities of the tissue-equivalent materials were also determined and compared with values available in the literature. Linear attenuation coefficients of 0.724 and 0.923 cm(-1) were determined, respectively, for adipose and glandular tissues. Such values agree with data available in the literature. On the basis of the results obtained in this work, it is suggested that BTE phantoms are used instead of polymethyl methacrylate phantoms to select exposure parameters (kV, mAs and target/filter combination) specific for breast glandularities from 0 to 50 % in the optimisation of doses in mammography. 相似文献