奇奇核158Ho和124Cs高自旋态的实验研究

奇奇核作为研究准质子和准中子间相互作用的独特侯选核，近年来，人们给予了越来越多的关注。奇奇核高j组态带中观测到的低自旋旋称反转现象(Signature inversion)已成为原子核高自旋态领域中一个十分活跃的研究课题。近十年来，一系列基于二准粒子加转子模型框架的计算结果表明，奇奇核中这两个准粒子之间的相互作用与旋称反转现象的发生密切相关。相对于偶偶核和奇A核，奇奇核的能级结构更复杂一些，实验上对其高自旋态的研究比较困难，这主要体现在实验上所提供的许多奇奇核的能级纲图存在着一定程度的不确定性，例如能级的激发能位置、转动带的组态、自旋和宇称的指定，甚至在纲图结构、级联系列的核素归属等方面都有一些问题。其中，转动带能级自旋的指定直接关系到准粒子能量的劈裂属性(即正常劈裂还是反常劈裂、旋称反转发生在低自旋区还是高自旋区及旋称反转的发生位置等)：自旋的奇偶性定错了，会导致本来是反转的旋称劈裂变成不反转的(反之亦然)；自旋值定错了△I，会导致旋称反转的位置发生相应的漂移。由于实验上奇奇核转动带能级自旋指定的混乱局面，掩盖了旋称反转现象的客观规律，使得相关理论模型的计算结果得不到及时检验。基于激发能系统学分析方法、以顺排角动量相加性为判据，我们曾对A～160轻稀土区的πhl_(11/2)direct X vi_(13/2)转动带(17个核素)和A～130过渡区的πh_(11/2)direct XVh_(ll/2)转动带(20个核素)进行了系统研究，对其中20个核的自旋数据提出质疑、并提出了相应的修正方案，在此基础上总结了两核区旋称反转现象的系统规律。利用激发能系统学方法指定奇奇核转动带的能级自旋，主要遵循以下三点原则：①自旋奇偶性：根据推转壳模型的描述，当准粒子处于优惠态(Favored)时、较非优惠态(Unfavored)具有更大的顺排角动量。这样，通过对转动带中两signature分支系列的i_x大小的比较，可以辅助推断能级自旋的奇偶性；②顺排角动量相加性：在忽略p-n剩余相互作用条件下，奇奇核中总的顺排角动量近似等于相邻奇A核中相应组态带提取的准粒子顺排角动量之和。这样，利用i_x对自旋值比较敏感的特点，可以推断出能级自旋取值的大致范围；③激发能系统性分析：由于集体转动反映大量核子的集体行为，少数核子的改变不会对这种运动产生明显影响，利用转动惯量的组态相关特性，在一组同位素或同中子素系列链中，对应一定内禀结构的转动带，随着质子数或中子数的均匀递增，能级能量应表现光滑的变化趋势(即不发生突变)。这三个方面基于不同角度、相对独立地指定转动带自旋。其结论的统一、往往可以给出正确的自旋数据。然而，必须指出的是：系统学分析过程是一种经验方法，并不具有严格的理论基础，上述的自旋修正以及总结出的旋称反转规律，必须得到实验核谱学测量的支持。基于这一思想，针对两核区，我们分别选择情况较为阿典型的奇奇核~(158)Ho和~(124)Cs进行了集中的实验测量。本论文的主要研究目标就是要建立两核中晕带与低激发态或基态的联系，找出原纲图中错误自旋指定的原因所在，验证系统学结论的有效性，并用旋称反转的实验规律性对理论模型的系统计算结果进行检验。(一)奇奇核~(158)58Ho高自旋态的实验研究在原子能研究院的HI-13串列加速器上，通过~(152)Sm(~(11)B，5nγ)~(158)Ho融合蒸发反应(束流轰击能E_(lab)=60 MeV)、对目标核~(158)Ho的高自旋态进行布居。探测阵列由八个高纯锗探测器构成，为了提高低能射线的收集效率，使用了一个平面型高纯锗探测器。分别进行了激发函数曲线测量、γ-γ-t符合测量和剩余放射性测量。数据反演后，两重符合总记数～120x10~6。实验结果概括如下：1．建立了基态带，组态指定为：{πh_(11/2)[523]7／2-direct Xvh_(9/2)[521]3／2~-}K~π=5~+；2．建立了一个强度仅次于晕带的强耦合带结构(亚晕带：yrare band)。通过转动参数、跃迁几率、顺排角动量、带交叉频率等特征参量的分析，其组态指定为：{πg_(7／2)[404】7／2]~+ direct X vi_(3／2)[651]3／2~+}K~π=5~+。 尽管该带带头附近的结构还不完整，但观测到了带内几条能级退激、分别贯入到晕带和基态带，从而将晕带和亚晕带同基态联系起来，固定了晕带和亚晕带中能级的激发能位置，并通过对这些连接跃迁多极性的分析，指定了两个带中的能级自旋和宇称；3.晕带(πh_(11/2)direct X vi~(13/2))向高自旋端拓展了7条能级，最高自旋态达到26h，激发 能4．9MeV。肯定了原纲图中不确定的617kev跃迁的存在和放置，观测到了反转点(I_(inv.)≈16h)，肯定了系统学研究对该核的自旋修正。基于本实验建立的连接关系，晕带中观测到的最低态(即70.8kev跃迁贯入能级)激发能为207．6kev，而对应该能级，原纲图中激发能为156．9kev。这意味着原能级纲图中，晕带向基态退激途径中漏掉了一个～5lkeV的"能隙"(Energy gap)，自旋差|△I|=3。根据晕带与退激5-同质异能态的跃迁(156．9kev)的快符合关系，该"能隙"至少由两个跃迁构成。该结果否定了原纲图中对晕带带头处理的三种可能性(①70．8kev为连接跃迁，其退激的能级为带头；②70．8kev为带内跃迁，156．9kev、5-同质异能态为带头：⑨70．8kev为带内跃迁，156．9kev、5-同质异能态为带头，但带头附近仍存在尚未观测的跃迁)。不确切的连接关系是过去实验中无法正确指定晕带自旋的原因；4．建立了一个强耦合的转动带结构，其能级间距(跃迁E_γ)随角动量的增加均匀递增，组态指定为{πh_(11/2)[523]7／2~-direct Xvh_(11/2)[505]11／2~-}K~π=9~+；同时，观测到了另一高K激发态退激到该转动带。其内禀结构指定为：{πg_(7／2)[404]7／2~+direct Xvh_(11/2)[505]1 l／2~-}K~π=9~-；5．建立了基于156．9 kev(I~π=5~-、T_(1/2)=29 ns)同质异能态上的转动带，该带观测完整，具有较强耦合的结构特点。其内禀准粒子轨道指定为：{πh_(11/2)[523]_(7／2)~-direct X vd_(3／2)[402]3／2~+}K~π=5~-，与处于较低激发能(67．3 kev)的2~-态(T_(1／2)=27 min．)构成了一对GM伙伴态。否定了过去的实验中把该态指定为{πg_(7/2)~2+direct Xvh_(9/2)[521]3／2~-}K~π=2~-组态；6．观测到了一个基于65．5 kev激发态的转动带，通过理论模型预言的带头激发能及转动参数与实验值的比较、考虑到其较弱的布居强度和很低的顺排角动量、以及较强耦合的结构特点， 其组态指定为： {πd~(5／2)[402]5／2~direct X vh_(9／2)[521]3／2~-}K~π=4~-。这一结果肯定了过去放射性测量中对处于较高激发能(139．2 kev)、T_(1／2)=1．85 ns、I~π=1~-激发态的讨论，即二者构成了一对GM伙伴态；7．建立了基于{πh_(11／2)[523]7／2~-direct X v_(7／2)[523]5／2~-}K~π=6~+激发态的强耦合转动带结构，其带头激发能为450．1 kev，与I~π=1~+、激发能为146．9 kev的同质异能态构成了一对GM伙伴态；8．在过去的放射性衰变测量中，提供了三个2~+激发态(激发能分别为117．7 kev、74．95 kev和316 kev)。其中两个2~+态(117．7和74．95 kev)同时指定具有{πh_(11／2)[523↑]7／2~-direct X vh_(9／2)[521↓]3／2~-}K~π=2~+组态。这里，我们指定1 17．7 kev的2~+激发态为{πg_(7／2)[404↓]7／2~+ direct X vi_(l3／2)[651↓]3／2~+}K~π=2+组态，即与本实验建立的亚晕带内禀激发态构成了一对GM伙伴态，而74．95 kev的2~+激发态指定为 {πh_(11/2)[523↑]7／2~-direct X vh_(9/2)[521↓]3／2~-}K~π=2~+组态，即与基态构成了一对GM伙伴态。基于本实验中K~π=9~+激发态的观测及其转动带的建立，我们指定激发能为3 1 6 kev的2~+激发态具有{πh_(11/2)[523↓]7／2~-direct X vh_(11/2)[505个]1 1／2~-}K~π=2~+组态，即这两个态构成了一对GM伙伴态；9．通过本实验、提供了~(158)Ho中各能态的跃迁强度和跃迁几率等数据。概括起来，奇奇核~(158)Ho的能级纲图大大完善了。综合本实验观测到的高自旋转动带结构和放射性测量中的部分激发态信息，我们可以整理出10对GM伙伴态，并提供了四个分别对应自旋平行和反平行耦合的GM能量漂移(GM Shift)，即：{πh_(ll／2)[523]7／2~-direct Xvh_(9／2)[521]3／2~-}K~π=5~+、2~+，EGM=101．4 kev；{πh_(11/2)[523] 7／2~-direct X vd_(3／2)[402]3／2~+}K~π=5~-、2~-，E_(GM)=64．1 kev；{πd_(5/2)[402]5／2~+direct X vh_(9／2)[521]3／2~-}K~π =4~-、1~-，E_(GM)=113．3 kev；{πh_(11/2)[523]7／2~-direct Xvf_(7/2)[523]5／2~-}K~π=6~+、1~+，EGM=255．7 keV。(二)奇奇核~(124)Cs高自旋态的实验研究在原子能院的HI-13串列加速器上，利用~（116）Sn（~（11)B，3nγ)~(124)Cs融合蒸发反应(束流轰击能E_(lab.)=45 MeV)，对奇奇核~(124)Cs的高自旋态进行了布居。探测阵列由10个高纯锗探测器和一个小平面探测器组成。数据反演后，总的两重符合事件数达到160x10~6。实验结果概括如下：1．高自旋转动带的信息更丰富了：建立了三个新的转动带结构，其中两个耦合带、一个退耦带，组态分别为：{πh_(11／2)[550]1／2~- direct X vhd_(5/2)[413]5／2~+}K~π=3~-、{πg_(7／2)[413]5／2~+direct X vg_(7/2)[402】5／2~+}K~π=5~+以及{πh_(11/2)[550]1／2~- direct X vd_(3/2)[400]l／2~+}K~π=1~-；2．低激发态的信息更丰富了：观测到了20多条新的低激发态跃迁，增加了10多个新的低激发态；3．转动带之间以及转动带与低激发态间耦合的信息大大丰富了：在过去的研究中观测到了三个彼此孤立、悬空的转动带结构，这里指定它们的组态为：{πh_(11／2) [550]1／2~-direct X vh_(11/2)[523]7／2~-}K~π=4~+(晕 带) ； {πh_(11/2)[550]1／2~- (direct X)vg_(7/2)[402]5/2~+}K~π=3~-(亚晕带：布居强度仅次于晕带)；{πh_(11/2)[550]1/2~-(direct X)vs_(1/2)[411]1／2~+}K~π=1~-(双退耦结构)。其中，亚晕带(yrare band)通过至少三个独立的退激路径与低激发态联系起来；同时，建立了晕带与亚晕带间的多条连接关系。其它转动带分别与晕带和亚晕带联系起来，从而，在奇奇核~(124)Cs中，转动带的"悬空"不再存在，限定了各转动带中能级的激发能位援，并通过这些连接跃迁多极性的分析，分别指定了各能态的自旋和宇称。4．基于本实验建立的连接关系，晕带的最低态(124kev射线贯入能级)的激发能为618．9kev，该能量值比过去研究中的同一能级高出11．7kev。这表明原能级纲图中晕带的退激途径漏掉了一个11．7kev的"能隙"(根据Weisskopf估计，该能隙很可能由两个偶极跃迁构成)。该"能隙"的漏观测，正是导致过去实验中无法正确指定晕带自旋的原因所在；

Heat capacity and thermodynamic properties of crystalline ornidazole (C7H10ClN3O3)

The molar heat capacities of 1-(2-hydroxy-3-chloropropyl)-2-methyl-5-nitroimidazole (Ornidazole) (C7H10CIN3O3) with purity of 99.72mol% were measured with an adiabatic calorimeter in the temperature range between 79 and 380K. The melting-point temperature, molar enthalpy Delta(fus)H(m), and entropy, Delta(fus)S(m), of fusion of this compound were determined to be 358.59 +/- 0.04K, 21.38 +/- 0.02 kJ mol(-1) and 59.61 +/- 0.05 J K-1 mol(-1), respectively, from fractional melting experiments. The thermodynamic function data relative to the reference temperature (298.15 K) were calculated based on the heat capacities measurements in the temperature range from 80 to 380 K. The thermal stability of the compound was further investigated by DSC and TG. From the DSC curve an intensive exothermic peak assigned to the thermal decomposition of the compound was observed in the range of 445-590 K with the peak temperature of 505 K. Subsequently, a slow exothermic effect appears when the temperature is higher than 590 K, which is probably due to the further decomposition of the compound. The TG curve indicates the mass loss of the sample starts at about 440K, which corresponds to the decomposition of the sample. (C) 2003 Elsevier B.V. All rights reserved.

科尔沁沙地22种菊科草本植物叶片形态特征研究

以内蒙古科尔沁沙地22种菊科草本植物为实验材料,研究这些植物的比叶面积、叶片厚度、叶片干物质含量、叶片体积、叶重比和叶片组织密度等特性之间的关系。结果表明,叶片体积和叶片厚度之间存在较强的正相关,其相关系数r=0.782。而叶片厚度与叶片组织密度、比叶面积与叶片组织密度、叶片体积与叶片组织密度之间则存在一定的负相关性,它们的相关系数分别为-0.767、-0.559和-0.505,其余各特性之间均不存在相关性。根据赋值后数据或者二元数据,运用聚类分析方法得出3个组群,并运用单因素方差分析方法检验各特性在各组间的显著性,叶片厚度、叶片体积、叶重比和叶片组织密度特性在组间存在极显著差异。

Microstructure and mechanical properties of Mg-4Al-4Nd-0.5Zn-0.3Mn alloy

Mg-4Al-4Nd-0.5Zn-0.3Mn alloy was prepared by metal mould casting method. Microstructure, aging behavior, mechanical properties and fracture morphology of the alloy were investigated. The results showed that alpha-Mg, Al-11 Nd-3, Al2Nd and Mg-32(Al,Zn)(49) phases were the main phases of the as-cast alloy. And the long rod-like Al-11 Nd-3 phase was decomposed to granular Al2Nd through T6 heat treatment. The tensile strength was also enhanced by T6 treatment. The yield strength was increased by 17% and 21% at RT and 150 degrees C, respectively. It was mainly because that the precipitates were refined through T6 treatment and this became more benefit to hinder dislocations slipping.

Preparation and luminescence properties of Mn2+-doped ZnGa2O4 nanofibers via electrospinning process

One-dimensional Mn2+-doped ZnGa2O4 nanofibers were prepared by a simple and cost-effective electrospinning process. X-ray diffraction (XRD), Fourier transform infrared spectroscopy (FT-IR), thermogravimetric and differential thermal analysis (TG-DTA), scanning electron microscopy (SEM), energy-dispersive X-ray spectrum (EDS), transmission electron microscopy (TEM), high-resolution transmission electron microscopy (HRTEM), photoluminescence (PL) and cathodoluminescence (CL) spectra as well as kinetic decays were used to characterize the samples. SEM results indicated that the as-formed precursor fibers and those annealed at 700 degrees C are uniform with length of several tens to hundred micrometers, and the diameters of the fibers decrease greatly after being heated at 700 degrees C. Under ultraviolet excitation (246 nm) and low-voltage electron beams (1-3 kV) excitation, the ZnGa2O4:Mn2+ nanofibers presents the blue emission band of the ZnGa2O4 host lattice and the strong green emission with a peak at 505 nm corresponding to the T-4(1)-(6)A(1) transition of Mn2+ ion.

交联型聚乙烯亚胺智能基因载体的制备及PEG化影响

使用胱胺双丙烯酰胺(CBA)对低分子量聚乙烯亚胺(PEI)进行交联反应制备智能降解型聚阳离子基因载体.通过与聚乙二醇(PEG)反应得到不同程度PEG化的聚阳离子载体.利用核磁、黏度测试、粒度仪、zeta电位仪和凝胶电泳对聚阳离子载体及其与DNA的复合物进行了表征.研究表明随着PEG含量的增加,聚阳离子载体/DNA复合物颗粒粒径变小、表面正电荷降低,PEG具有明显的屏蔽作用,但过多的PEG也使载体与DNA复合能力下降.通过MTT细胞毒性测试和荧光素酶质粒转染实验得出,含二硫键的交联型阳离子聚合物在测试范围内显示了非常低的细胞毒性,最佳转染效率是PEI25k的4倍,PEG化后其细胞毒性得到进一步改善,转染效率却明显降低.

SYNTHESIS AND CHARACTERIZATION OF A CROSSLINKING POLYETHYLENIMINE AS SMART GENE CARRIER AND EFFECTS OF PEGYLATION DEGREE

A smart biodegradable cationic polymer (CBA-PEI) based on the disulfide bond-containing cross-linker cystamine bisacrylamide (CBA) and low molecular weight branched polyethylenimine (1800-Da, PEI1800) was successfully synthesized by Michael addition reaction in our recent study. Furthermore, a series of copolymers (CBA-PEI-PEG) with different PEGylation degree were obtained by the mPEG-SPA (5000-Da) reacting with CBA-PEI at various weight ratios directly. The molecular structures of the resulting polymers CBA-PEI and CBA-PEI-PEG were evaluated by nuclear magnetic resonance spectroscopy (H-1-NMR) and capillary viscosity measurements, all of which had successfully verified formation of the copolymers. The polymer/DNA complexes based on CBA-PEI and CBA-PEI-PEG were measured by dynamic light scattering and gel retardation assay. The results showed that the particle size and zeta potential of complexes were reduced with increasing amount of PEG grafting, even no particle formation. The particle size of CBA-PEI/DNA complexes was in range of 103.1 to 129.1 nm, and the zeta potential was in range of 14.2 to 24.3 mV above the 2:1 weight ratio. In the same measure condition, the particle size of CBA-PEI-PEG complexes was reduced to a range of 32.2 to 55 nm, and the zeta potential was in range of 9.3 to 13.8 mV at the 2:1 weight ratio.

Microstructures and mechanical properties of extruded Mg-8Gd-0.4Zr alloys containing Zn

Microstructures and mechanical properties of the Mg-8Gd-xZn-0.4Zr (x = 0, 1 and 3 wt.%) alloys in the as-cast, as-extruded and extruded-T5 conditions, have been investigated. The peak-aged Mg-8Gd-1Zn-0.4Zr alloy during isothermal ageing at 423 K acquires highest mechanical properties, with the highest ultimate tensile strength and yield tensile strength of 314 and 217 MPa, respectively. Addition of Zn has obvious effect on age hardening responses, especially for 1 wt.% Zn addition. It is due to a uniform distribution of beta' phase which can impede the movement of dislocations. However, addition of 3 wt.% Zn to the Mg-8Gd-0.4Zr alloy leads to a precipitation of Mg3Zn3Gd2 phase (W-phase). This phase is incoherent with interface of the matrix and becomes cores of the fracture in tensile test at room or elevated temperature.

Citrate-gel synthesis and luminescent properties of ZnGa2O4 doped with Mn2+ and EU3+

By using inorganic salts as raw materials and citric acid as complexing agent, spinel oxide ZnGa2O4 and Mn2+, Eu3+-doped ZnGa2O4 phosphor powders were prepared by a citrate-gel process. X-ray diffraction (XRD), TG-DTA, FT-IR. and luminescence excitation and emission spectra were used to characterize the resulting products. The results of XRD reveal that the powders begin to crystallize at 500 degreesC and pure ZnGa2O4 phase is obtained at 700 degreesC, which agrees well with the results of TG-DTA and FT-IR. In the crystalline ZnGa2O4, the Eu shows its characteristic red (615 nm, D-5(0)-F-7(2)) emission with a quenching concentration of 5 mol% (of Ga3+), and the Mn shows green emission (505 nm, T, A,) with a quenching concentration of 0.1 mol% (of Zn2+). The luminescence mechanism of ZnGa2O4:Mn2+/Eu3+ is presented.

A novel one-dimensional manganese phosphomolybdate with rectangular cavities: [H3N(CH2)(4)NH3] (H3O)(2){[Mn(phen)(2)](4) [(MnMo12O30)-O-v(HPO4)(6)(H2PO4)2} center dot 4H(2)O

A novel manganese phosphomolybdate, [H3N(CH2)(4)NH3](H3O)(2){[Mn(phen)(2)](4)[(MnMovO30)-O-12(HPO4)(6)(H2PO4)(2)]} . 4H(2)O 1, has been hydrothermally synthesized and structurally characterized by single crystal X-ray diffraction. The crystal data: triclinic, P (1) over bar, a = 14.172(7) Angstrom, b = 16.547(2) Angstrom, c = 16.679(3) Angstrom, alpha = 62.881(12)degrees, beta = 73.83(3)degrees, gamma = 88.81(3)degrees. X-ray crystallography shows that the [Mn(phen)(2)] fragments are covalently bonded to the [Mn(Mo6P4)(2)] dimers leading to a one-dimensional chain with rectangular cavities occupied by tetramethylene-diamine cations and water molecules. (C) 2002 Elsevier Science B.V. All rights reserved.

Study on a novel polyimide precursor prepared by a modified polymerization of monomeric reactants (MPMR) procedure

A novel polyimide precursor based on the dimethyl ester of 3,3',4,4'-biphenyltetracarboxylic acid, 4,4'-methylene dianiline and the monomethyl ester of 5-norbornene-2,3-dicarboxylic acid (BPDE/MDA/NE) was prepared by a modified polymerization of monomeric reactants (PMR) approach (MPMR). The composition of the precursor was quantitatively characterized by means of FTIR, HPLC and GC. The fractions of imide, amic ester and amic acid units in the precursor, typically prepared by refluxing in 1,4-dioxane for 2 h, were 33.7, 30.8 and 1.1 mol-%, respectively. The portion of free MDA was 3.34 wt.-% as determined by HPLC.

Synthesis, electrochemistry, and fluorescence of two Ru(phen)(3)(2+)-based surfactants

Two new Ru(phen)(3)(2+)-based surfactants, Ru(phen)(2)(phenNHCO-C-11)(PF6)(2) and Ru(phen)(2)(phenNHCO-C-17)(PF6)(2), have been designed and synthesized, whose chemical structures were characterized by means of IR, H-1 NMR and MS. Also, electrochemistry and fluorescence of them are reported.

镧离子对tRNA~(Phe)结构的影响:亚胺质子NMR谱

采用1HNMR方法研究了镧离子对酵母tRNAPhe分子结构和构象变化的影响 .结果表明位于扩大二氢尿嘧啶螺旋 (D 螺旋 )的端梢三级碱基对 (G_15) (C_4 8)明显受加入La3+ 的影响 ,向低场位移 0 33;与三级相互作用相关 ,连接D 茎和接受茎起固定L结构转折的 (U_8) (A_14)碱基对向高场位移 0 2 0 ;另一可能受La3+影响的亚胺质子碱基对为 (G_19) (C_56 ) ,由于该碱基对位于高度叠加的 12 6和 12 2之间 ,其归属仅供参考 ,该碱基对有助于D 环对TΨC环的连接.

Studies on the electron transfer centers of amino oxidase immobilized on self-assembly monolayer using electrochemical methods

The direct electron transfer of amino oxidase on electrode surface based on self-assembly technique occurs at 505 mW(vs. Ag/AgCl), indicating that copper atoms are the electron transfer centers and catalytic centers of amino oxidase.