共查询到16条相似文献,搜索用时 62 毫秒
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采用自制的催化剂和自行设计的高效催化反应器,用催化加氢的方法,以Ba13CO3为原料制备了13C-甲醇。所得甲醇水溶液在微型高效精馏反应器中进一步提纯后,得到的13C-甲醇化学纯度>99.5%。实验设计的合成路线反应条件温和,同位素利用率>90%。13C-甲醇经色质联用(GC-MS)和核磁(1H NMR)检测,13C同位素丰度>97%,13C-甲醇的同位素丰度与原料相比降低<1%。以上结果表明,采用自制的催化剂和自行设计的高效催化反应器,成功地用催化加氢的方法,制备得到了13C-甲醇。 相似文献
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本工作对低温精馏分离13C同位素的稳态模拟与动态模拟进行了研究。使用商用流程模拟软件Aspen Plus建立低温精馏过程的稳态模型,通过对比模拟数据与实验数据,验证物性参数和模型的可靠性。使用Aspen Dynamics建立低温精馏过程的动态模型,动态模拟结果与实验数据吻合良好。结果表明,可以使用Aspen Dynamics对碳同位素分离过程进行动态特性研究,并对精馏过程进行开车时间预测、控制方案分析、操作性分析和安全性分析等。 相似文献
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血管新生是肿瘤生长、转移过程中不可缺少的生物过程。整合素αⅤβ3受体在新生血管内皮细胞和多种肿瘤细胞表面高表达,在肿瘤血管新生中起着关键作用,目前已成为肿瘤诊断与治疗的一个重要靶点。精氨酸-甘氨酸-天冬氨酸(Arg-Gly-Asp, RGD)肽可特异性地与整合素αⅤβ3受体结合,18F标记的RGD肽类化合物PET显像可无创、动态地定量监测整合素αⅤβ3受体表达,在肿瘤早期诊断、疗效监测及抗血管新生评价上发挥着重要作用。本文就近年来国内外18F标记RGD 肽在肿瘤αⅤβ3受体显像中的研究进展作简要综述。 相似文献
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利用X射线衍射技术分析LaNi5氚老化效应 总被引:1,自引:0,他引:1
利用覆膜法对长期贮存氚的LaNi_5进行了XRD分析.经过实验发现,老化后的LaNi_5的谱峰比新鲜的LaNi_5存在明显的展宽,而经过高温除He处理后,又恢复到新鲜的LaNi_5水准,氚衰变形成的~3He在晶格中居留并在其中形成部分位错亚结构,这可能是导致LaNi_5 XRD衍射峰宽化的主要原因. 相似文献
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99Tcm-DTPA-DG标记物的制备 总被引:5,自引:0,他引:5
为了在合成二乙三胺五乙酸-脱氧葡萄糖(DTPA-DG)基础上,制备99Tcm-DTPA-DG标记物,以SnCl2·2H2O为还原剂,还原99TcmO-4并与DTPA-DG形成99Tcm-DTPA-DG标记物。进行了DTPA-DG用量、SnCl2·2H2O用量、反应介质pH值、反应温度等对标记率的影响实验。结果表明,25mg DTPA-DG ,500μg SnCl2·2H2O,pH=6,加入Na99TcmO4淋洗液0.5~4mL,在25℃以上放置30min或沸水浴反应10min时,用9g/L NaCl和丙酮作展开剂纸层析法鉴定标记物,放射化学纯度>99%。标记物在室温放置6h,放射化学纯度仍达98.6%。99Tcm-DTPA-DG标记率高,标记物的体外稳定性好,操作简便,便于临床应用。 相似文献
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肿瘤增殖显像剂18F-FLT的合成和标记 总被引:2,自引:0,他引:2
为制备肿瘤增殖显像剂3'-脱氧-3'-氟胸腺嘧啶脱氧核苷(3'-deoxy-3'-fluorothymidine, 18F-FLT),合成了标记前体3-N-t-叔丁氧羰基-1-[5'-O-(4, 4'-二甲氧基三苯甲基)-2'-脱氧-3'-O-(4-硝基苯磺酰基-β-1)-苏戊呋喃糖]胸腺嘧啶脱氧核苷(N-BOC-FLT)并进行了标记.标记前体和各步合成中间体均经红外、核磁共振和质谱确证;于120 ℃进行亲核氟化反应,标记率为(35.2±5.8)%(经校正,n=2),用TLC和HPLC检测其放化纯度(RCP)大于95%,可满足临床研究的要求. 相似文献
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对粉末样品进行压片制样,建立了能量色散X射线荧光(EDXRF)谱仪测定环境土壤样品中40K放射性活度的方法。方法标准曲线的相关系数为0.991 0,测量的精密度为2.98%,测量标准样品的最大相对偏差为6.40%。采用本方法和γ谱仪同时测量7个土壤样品,并对这两种分析方法的测量结果采用配对t检验SPSS程序计算。结果表明,两种方法所得数据无显著性差异(P>0.05),可使用X射线荧光谱仪法分析土壤中40K的放射性活度。这种方法操作简便,精密度和准确度较好,具有广泛的实用性。 相似文献
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A. Meftah W. AssmannN. Khalfaoui J.P. StoquertF. Studer M. ToulemondeC. Trautmann K.-O. Voss 《Nuclear instruments & methods in physics research. Section B, Beam interactions with materials and atoms》2011,269(9):955-958
The results of present paper have shown that sputtering of yttrium iron garnet (Y3Fe5O12) under swift heavy ions in the electronic energy loss regime is non-stoichiometric. Here we are presenting additional experimental results for gadolinium gallium garnet (Gd3Ga5O12) as target. The irradiations were performed with different ions (50Cr (589 MeV), 86Kr (195 MeV) and 181Ta (400 MeV)) impinging perpendicularly to the surface. As earlier, the sputtering yield was determined by collecting the emitted gadolinium and gallium atoms on a thin aluminium foil, placed upstream above the target and analyzing the Al catcher by Rutherford backscattering. Also for Gd3Ga5O12, the emission of Gd and Ga is non-stoichiometric. Sputtering appears above a critical electronic stopping power of Sth = 11.6 ± 1.5 keV/nm, which is larger than the threshold for track formation, in agreement with other amorphisable materials. In addition, the angular distribution of the sputtered species was measured for Y3Fe5O12 and Gd3Ga5O12 using 200 MeV Au ions impinging the surface at 20° relatively to the surface. For the two garnets the ratio of Y/Fe (and Gd/Ga) varies with the angle of emitted species and the stoichiometry seems to be preserved only for an emission perpendicular to the surface. 相似文献
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Oscar A. Restrepo Aneesh PrabhakaranArnaud Delcorte 《Nuclear instruments & methods in physics research. Section B, Beam interactions with materials and atoms》2011,269(14):1595-1599
Using molecular dynamics simulations (MD), this contribution compares the interaction of three energetic clusters (Au3, Au400 and C60) with a hybrid surface of crystalline polyethylene (PE) covered by a layer of gold nanoparticles. This model system mimics the situation encountered in metal-assisted secondary ion mass spectrometry. The chosen impact points are representative of the PE surface, the metal particles and the frontier between the metal and the polymer. The simulations show the differences between the impact over the Au nanoparticle and the polymer surface, in terms of projectile penetration, crater formation and sputtering yield of PE and gold species. For C60 and Au3 projectiles, a simple correlation is found between the quantity of energy deposited in the top polymeric layers and the quantity of sputtered polymer material, including all the impact points. The results obtained with Au400 do not fit on this line, indicating that other physical parameters are prevalent. The mechanistic view of the interaction provided by the MD helps explain the differences. In short, while C60 and Au3 quickly break apart, creating energetic recoils and severing many bonds in the surface, Au400, with the largest total momentum by far (∼10 times larger than the others) and the lowest energy per atom (25 eV), tends to act and implant in the solid as a single entity, pushing the polymeric material downwards and breaking few bonds in the surface. 相似文献