208 resultados para (H, G)-coincidence


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本文采用自行设计的均速增加加热电压改变元件温度的方法以及动、静态气敏特性测试方法并借助其它测试手段(X光衍射、BET、扫描电流)系统地研究了表面电导控制型SnO_2系元件和体电导控制型γ-Fe_2O_3元件在变温过程中与H_2O(g)、O_2(g)和还原性气体相互作用的规律。实验结果表明:添加剂Al_2O_3、MgO、Pd、Pt和Sb_2O_3均对元件的体电阴均有调制作用。Al_2O_3是以微粒状存在于元件内,它为元件提供了活化中心,提高了元件的灵敏度。而γ-Fe_2O_3具有超微细结构。SnO_2系元件和γ-FeO_3元件取样电压(V_L)与温度(T)的变化关系在空气和惰性气氛中均是非线性的。材料组份不同的元件,其V_L~T变化规律不同。各元件在空气和惰性气氛中的变化,除阻值不同外,其V_L~T变化规律基本相同。综合考虑添加剂(Al_2O_3、MgO)和气氛(空气、惰性气氛、纯氧气)的影响,SnO_2系元件的V_L~T变化规律不仅是由于氧在元件表面上的吸附及吸附状态的不同所引起,很大程度上取决于元件材料的组成和温度对材料内载流子浓度和逐移率的影响。基于对SnO_2系元件的V_L~T变化规律的分析,γ-Fe_2O_3元件V_L随温度的变化也是由于环境中的氧和材料内载流子迁移率随温度的变化所致。SnO_2系元件和γ-Fe_2O_3元件在不同温度所测的V_L~T变化关系表明:SnO_2元件在低温(<72%RH)条件下,具有与干燥空气中相同的V_L~T变化关系;在高温度(>72%RH)的空气中,H_2O(g)的存在对元件低温区(<100 ℃) (200 ℃-400 ℃)的V_L值均有影响,在低温区的V_L值较干燥空气中的V_L值高;中温区的V_L值较干燥空气中的V_L值低。把在约98%RH的空气和氩气中的V_L~T变化曲线比较表明:中温区的实验现象是由于空气中H_2O(g)与O_2(g)共存所致。γ-Fe_2O_3元件在不同温气气氛中的V_L~T变化规律相同,且在元件工作温度(129 ℃~320 ℃)范围内V_L值相同,但均较干燥空气中该条件下的V_L值高。在实验中亦观察到SnO_2元件在温度低于72%RH中长期放置亦可观察到与实验中温度>72%RH条件下相同的V_L~T变化。SnO_2元件在空气和惰性气氛中对还原性气体均有气敏性。而且在惰性气氛中对微量还原性气体(H_2)的灵敏度比在空气中的灵敏度高。掺贵金属Pd或Pt的SnO_2元件在惰性气氛中,当H_2浓度高于8000ppm时,元件电导突变式增加。我们认为SnO_2系元件在空气中检测还原性气体的工作机理是表面化学反应过程;在惰性气氛中其工作机理是表面解离吸附过程。γ-Fe_2O_3元件在空气中对C_4H_(10)具有较高的选择性。但在惰性气氛中对还原性气体不具有气敏性。我们认为环境中氧是体电导控制型气敏元件气敏性不可缺少的中间媒介。其检测机理是微观可逆氧化-还原过程。

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:与其姐妹科(菊头蝠科)相比,蹄蝠科的细胞遗传学研究较少。迄今为止,仅少数蹄蝠科几个物种有高分辨率的G带核型报道,且有关该科核型进化的大多数结论都是基于常规Giemsa染色研究而得。该研究利用三叶小蹄蝠的染色体特异探针,通过比较染色体涂色、G和C显带,建立了5种蹄蝠的染色体同源性图谱,并探讨了它们同源染色体间的G和C带异同。结果表明:罗伯逊易位、臂内倒位以及异染色质的扩增可能是蹄蝠科物种核型进化的主要机制。通过对这5种蹄蝠物种及其外群物种之间的同源染色体片段的比较分析,作者推测蹄蝠科的祖先核型并不像先前认为的全由端着丝粒染色体组成, 而应该含有中着丝粒染色体。

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利用时间分辨Kerr旋光技术测量低温下稀磁半导体Ga_(0.937)Mn_(0.063)As中光注入极化载流子的自旋进动信号,并观察到自旋极化载流子的有效g因子值随外磁场的增强而增大的反常现象.这归结于磁场导致局域化空穴转化为非局域化空穴,从而使自发磁化强度增强,有效g因子值增大.基于此物理图像,进一步给出了(Ga,Mn)As的有效g因子与外磁场的关系式.

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Undoped, Zn-doped and Te-doped GaSb with different concentrations were investigated by positron lifetime spectroscopy (PAS) and the Doppler broadening technique. Detection sensitivity of the latter technique was improved by using a second Ge-detector for the coincident detection of the second annihilation photon. PAS measurement indicated that there were vacancies in these samples. By combining the Doppler broadening measurements, the native acceptor defects in GaSb were identified to be predominantly Ga vacancy (V-Ga) related defects.

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本文筛选一株苏芸金杆菌与氧化葡萄糖酸杆菌组成的新组合菌G. B529,并对其生物学性质进行研究,结果表明:新组合菌的摇瓶发酵转化率较原菌系提高4.83个百分点,发酵速度快,且具有耐受高浓度(10%)山梨糖的特性。为使G. B529的潜能得到最大程度的发挥,对其影响因素进行研究。首先应用均匀设计方法确立了G. B529的发酵培养基优化配比,在所实验的范围内,发酵转化率与玉米浆浓度成正相关性,尿素浓度 1.45%佩W/V)时,转化率达最大。其次种液各参数对发酵影响实验确立了判断种子质量高低的方法。结果显示种液中的大菌OD值一1.6 X小菌OD值可以作为种液的质量指数。最后对种子质量的影响实验显示适当提高玉米浆、葡萄糖等成分的浓度与降低尿素的浓度及调高pH值均有利于种液质量的改善。同时低接种量、大通气量和选择种龄为14小时均有助于种液质量指数的提高。 新组合菌系在选定的条件下枷3罐中4批发酵显示出很强的发酵能力,平均醇酸转化率较对照提高8.16个百分点,周期缩短10.6小时。其在300M3罐中生产试用行,连续26批次的平均醇酸转化率达87.40%,较生产用菌提高3.32个百分点。平均周期也缩短1.3小时。

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The first spectroscopic study for the beta decay of N-21 is carried out based on beta-n, beta-gamma, and beta-n-gamma coincidence measurements. The neutron-rich N-21 nuclei are produced by the fragmentation of the E/A=68.8 MeV Mg-26 primary beam on a thick Be-9 target and are implanted into a thin plastic scintillator that also plays the role of beta detector. The time of flight of the emitted neutrons following the beta decay are measured by the surrounding neutron sphere and neutron wall arrays. In addition, four clover germanium detectors are used to detect the beta-delayed gamma rays. Thirteen new beta-delayed neutron groups are observed with a total branching ratio of 90.5 +/- 4.2%. The half-life for the beta decay of N-21 is determined to be 82.9 +/- 7.5 ms. The level scheme of O-21 is deduced up to about 9 MeV excitation energy. The experimental results for the beta decay of N-21 are compared to the shell-model calculations.

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A full-ring PET insert device should be able to enhance the image resolution of existing small-animal PET scanners. Methods: The device consists of 18 high-resolution PET detectors in a cylindric enclosure. Each detector contains a cerium-doped lutetium oxyorthosilicate array (12 x 12 crystals, 0.72 x 1.51 x 3.75 mm each) coupled to a position-sensitive photomultiplier tube via an optical fiber bundle made of 8 x 16 square multiclad fibers. Signals from the insert detectors are connected to the scanner through the electronics of the disabled first ring of detectors, which permits coincidence detection between the 2 systems. Energy resolution of a detector was measured using a Ge-68 point source, and a calibrated 68Ge point source stepped across the axial field of view (FOV) provided the sensitivity profile of the system. A Na-22 point source imaged at different offsets from the center characterized the in-plane resolution of the insert system. Imaging was then performed with a Derenzo phantom filled with 19.5 MBq of F-18-fluoride and imaged for 2 h; a 24.3-g mouse injected with 129.5 MBq of F-18-fluoride and imaged in 5 bed positions at 3.5 h after injection; and a 22.8-g mouse injected with 14.3 MBq of F-18-FDG and imaged for 2 h with electrocardiogram gating. Results: The energy resolution of a typical detector module at 511 keV is 19.0% +/- 3.1 %. The peak sensitivity of the system is approximately 2.67%. The image resolution of the system ranges from 1.0- to 1.8-mm full width at half maximum near the center of the FOV, depending on the type of coincidence events used for image reconstruction. Derenzo phantom and mouse bone images showed significant improvement in transaxial image resolution using the insert device. Mouse heart images demonstrated the gated imaging capability of the device. Conclusion: We have built a prototype full-ring insert device for a small-animal PET scanner to provide higher-resolution PET images within a reduced imaging FOV. Development of additional correction techniques are needed to achieve quantitative imaging with such an insert.