28 resultados para <2 µm, >9 phi

em Chinese Academy of Sciences Institutional Repositories Grid Portal


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The reactions of [Cp2Mo2(CO)4] (1) with 2,2'-dipyridyl disulphide (C5H4NS-)2, 8,8'-diquinolyl disulphide (C9H6NS-)2 and tetramethyl thiuram disulphide (Me2NC(S)S-)2 in toluene solution resulted in the cleavage of the Mo-Mo triple bond to yield molybdenum complexes [CpMo(CO)2(C5H4NS)] (2), [CpMo(CO)2(C9H6NS)] (3) and [CpMo(CO)2(S2CNMe2)] (4), respectively. The molecular structures of 2, 3 . O=PPh3 and 4 were determined by X-ray diffraction studies. Crystals of 2 are monoclinic, space group P2(1)/n, with Z = 4, in a unit cell of dimensions a = 6.448(1), b = 12.616(2), c = 14.772(2) angstrom, beta = 92.85(1)-degrees. The structure was refined to R = 0.028 and R(w) = 0.039 for 1357 observed reflections. Crystals of 3 . O=PPh3 are triclinic, space group P1BAR, with Z = 2, in a unit cell of dimensions a = 11.351(3), b = 13.409(3), c = 9.895(2) angstrom, alpha = 94.59(2), beta = 90.35(2), gamma = 78.07(2)-degrees. The structure was refined to R = 0.033 and R(w) = 0.037 for 3260 observed reflections. Crystals of 4 are monoclinic, space group P2(1)/a and Z = 4 with a = 12.468(5), b = 7.637(2), c = 13.135(4) angstrom, beta = 96.62(3). The structure was refined to R = 0.032 and R(w) = 0.042 for 1698 observed reflections. Each of complexes 2-4 contains a cyclopentadienyl ligand, a cis pair of carbonyls and a chelate ligand (S,N donor or S,S donor). All the compounds have distorted square-pyramid structures.

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Medium-spin states of Ge-70 have been studied via the Ni-60(C-12,2p gamma)Ge-70 reaction at 45 MeV. The ground-state band and the second 0(+) band have been extended to the 12(+) and 8(+) states, respectively. Two negative-parity bands, one of which has a coupled structure and the other has a decoupled structure, have been observed additionally. Although the latter decoupled structure was known up to the (21(-)) state from a previous experiment, the part of the level scheme up to the 15(-) state has been largely modified by the present experiment. Backbendings observed in the positive- and negative-parity yrast bands have been compared with those of the neighboring even Ge isotopes. The experimental level structure has been compared with the shell-model calculations in the model space (2p(3/2), 1f(5/2), 2(p1/2), 1g(9/2)) employing two kinds of effective interactions, one of which is an extended P + QQ interaction with monopole interactions and the other is developed from a renormalized G matrix. Microscopic structures of the observed bands have been discussed with the help of the shell-model calculations.

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利用溶胶 凝胶法低温合成了BaCe0 .8Ln0 .2 O2 .9(Ln =Gd ,Sm ,Eu)固体电解质 ,X射线粉末衍射表明 90 0℃即形成正交钙钛矿结构 ,较高温固相反应合成温度降低了约 6 0 0℃ .测定了样品的阻抗谱和电导率 ,研究了其导电机理 ,溶胶 凝胶法合成可减小或消除固体电解质的晶界电阻 ,80 0℃时BaCe0 .8Gd0 .2 O2 .9的σ =7.87× 10 -2S·cm-1,以它为电解质的氢氧燃料电池开路电压接近 1V ,最大输出功率密度为 30mW·cm-2 .

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万家寨引黄工程隧洞总干线~#7隧洞位于偏关县葛家山至水泉河间,总长约9.21km,其中土洞长2.685km,隧洞开挖直径6.012m,衬砌内径5.46m,衬砌厚0.25m,每环由4块六角形管片组成,管片与洞壁间用豆砾石灌浆回填。~#7隧洞部分穿过地质年代为第四纪(Q3)黄土,其颗粒组成和物理性质指标见表1,2。土名为黄土状粉土。为分析计算隧洞和管片在周围土体作用下,及在通水和放空情况下的应力和变形情况,对~#7土洞进行有限元分析。在确定的c,#phi#值时,分别取原状土进行了卸载、加载试验,并计算出邓肯-张模型中的k,n,R_f,G,F,D进行比较。文中还对用两种试验获得的模型参数进行有限元变形分析的结果进行比较。

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由通式(Ⅰ)所示的N-取代基-4-取代苯基-5-烷基-5-取代苄基吡咯烷酮-2类化合物,具有钙拮抗活性,可应用于制备治疗脑功能障碍病药物,早老性痴呆病药物,增强学习记忆药物。其中R1是氢,取代苯甲酰基,1—5个碳原子的链状酰基。R2是氢,1—10个碳原子的正、异构烷基。X是氢,邻、间、对位取代的氟、氯、溴原子或甲氧基、乙氧基。吡咯烷酮-2环上的4,5-二或三取代包括顺式(RS及SR)构型、反式(SS)及RR构型。合成通式(Ⅰ)及其吡咯烷酮-2的方法。通式(Ⅰ)如上。

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结果显示 :当年草鱼种和中华鳖脾细胞培养上清液中能检测出IL 2活性 ,而且 1龄以上草鱼、中华鳖的IL 2活性高于当年孵化的草鱼和中华鳖。草鱼、中华鳖脾细胞在 2 5℃培养温度条件下 ,其上清液中IL 2活性最高 ,35℃次之 ,1 5℃最低。因此 ,草鱼、中华鳖IL 2活性在一定范围内是随着年龄增加而增强和依赖温度的。通过小鼠胸腺细胞增殖和对小鼠L92 9细胞杀伤率的实验表明 37℃比 2 5℃检测温度下所测的IL 2活性高 ,而中华鳖胸腺细胞增殖实验却显示 2 5℃检测温度下IL 2活性高于 37℃

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本论文合成了R_1Ba_2Cu_3O_(2-x) (R = La、Nd、Sm、Eu、Gd、Dr、Ho、Er、Tm、Yb)、Y_2Ba_2Cu_3O_(2-x) (x = 0.10~1.17)和Y_1Ba_2Cu_3O_(7-x)S_x (x = 0~2),并对磁性和超导电性进行了较为系统的研究。R_1Ba_2Cu_3O_(2-x)的磁化率在T > Tc的很宽的温度范围内服从Curic-Weiss定律,求得的有效磁矩略大于理论值,差值与Y_1Ba_2Cu_3O_(2-x)中Cu~(2+)磁矩相近,说明Cu~(2+)的磁矩对体系磁性有额外贡献,这贡献随R~(3+)离子中自旋平行的电子权的增多而增大。其高温下的磁化率CT > 700K)相对Curic-Weiss定律发生较大偏离,这偏离可能的来源有三个:高温下稀土离子发生较大的能级反转效应,高温下结构相变对磁性的影响,高温下氧含量减少造成Cu~(2+)磁矩增大。R_1Ba_2Cu_3O_(2-x)磁化率在T < Tc时也服从Curic-Weiss定律,R~(3+)磁矩是定域的,表明超导与磁性相互独立。互不相关,稀土磁矩与传导电子间无相互作用。用Sr取代R_1Ba_2Cu_3O_(2-x)中的Ba,没能使体系产生磁有序的变化,但却使有效磁矩增大,并完全破坏了样品的超导电性。Sm~(3+)磁化率不服从Curic-Weiss定律,在Sm_1Ba_2Cu_3O_(2-x)中Sm~(3+)显示了典型Van VlccK离子的特性。Y_1Ba_2Cu_3O_(2-x)随氧含量减少发生超导体一半导体一绝缘体的转化,当氧含量由6.90减小至6.49时发生由正交到四方的结构相变。当(7-x) = 5.83时有较多杂质相出现,123相开始分解。样品磁化率均服从Curic-Weiss定律,并随氧含量增大磁化率-温度曲线越来越趋于平缓(直线),当(7-x) = 6.90时磁化率基本不随温度变化,这时Pauli顺磁性占主导地位,这说明氧含量增加定域磁矩减少,求得的有效磁矩Peff随氧含量增大总趋势减小。提出了电子“巡游”的观点,较好地解释了上述现象,并推测出Cu(2)的d电子是离域的,对样品磁矩没有贡献,样品Peff来源于部分Cu(1)的定域Cu~(2+)的磁矩,上述推测被EPR结果证实。正交相Y_1Ba_2Cu_3O_(2-x)的EPR谱显示了中心对称成准立方晶场中Cu~(2+)(d~9, S = 1/2, I = 3/2)的EPR物性。而四方相样品的EPR谱却出现了明显的各向异性,说明观察到的为Cu(1)的EPR信号,由Cu(1)~(2+)的写域磁矩产生。Y_1Ba_2Cu_3O_(2-x)的EPR信号束源于本体相,而非Y_2Cu_2O_5、BaCuO_2、Y_2BaCuO_5等杂质相。各样品EPR信号的自旋浓度远小于1spin/cu,并随氧含量减小而增大,当(7-x) = 6.49、6.40时自旋浓度出现陡增,这时伴随由正交到四方的转化,证明了电子“巡游”观点的正确。用硫部分取代Y_1Ba_2Cu_3O_2g中的氧,当Y_1Ba_2Cu_3O_(2-x)Sx中x = 0.11时Tc = 92.6K,比Y_1Ba_2Cu_3O_(7-x)升高2K,但由于杂质相的存在,ΔTc加宽。其他样品多为半导体和绝缘体。硫取代0,当x = 0.04,0.06,0.11和1.20时磁化率服从Curic-Weiss定律,并且x = 0.87,1.2时分别在230K、240K出现反铁磁有序。其他样品由于Cu被还原为+1价而变成抗磁性。x = 0.11 (Tc = 92.6K),EPR谱为正交场中Cu~(2+)的信号。自旋浓度与温度无关。当所有Cu均为Cu~(1+)时,测问的是-s-的EPR信号,而Cu为混合价态(+1和+2时)测问是上述两种信号的叠加。

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To evaluate the radiative electron capture for the collisions of U89+ ion with N-2, radiative recombination cross sections and the corresponding emitted photon energies are calculated from the ground state 1s(2)2s to 1s(2)2snl(j) (2 <= n <= 9, 0 <= l <= 6) using the newly developed relativistic radiative recombination program RERR06 based on the multiconfiguration Dirac-Fock method. The x-ray spectra for radiative electron capture in the collision have been obtained by convolving the radiative recombination cross sections and the Compton profile of N2. Good agreement is found between the calculated and experimental spectra. In addition, the transition energy levels and probabilities among the 147 levels from the captured 1s(2)2snl(j) have been calculated. From the calculated results, radiative decay cascade processes followed by the radiative electron capture have also been studied with the help of multistep model and coupled rate equations, respectively. The present results not only make us understand the details of the radiative electron captures and the radiative decay cascade spectra in the experiment but also show a more efficient way to obtain the cascade spectra. Finally, the equivalence between the multistep model and coupled rate equations has been shown under a proper condition and the latter can hopefully be extended to investigate other cascade processes.

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用离子交换法制备了Mn2+交换的NaY分子筛MnNaY,用红外光谱(IR)和X射线粉末衍射(XRD)等方法进行了表征.研究了Mn2+含量为3.2%的样品在酸性水溶液中的稳定性和离子交换选择性.弛豫时间测量和体内磁共振成像实验表明其弛豫效率变化范围为4.9~9.7mmol·L·s-1,高于目前临床所用造影剂Gd-DTPA,对胃部MRI信号具有良好的增强效果.它是比较好的潜在口服胃肠道造影剂.

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Reactions of freshly prepared M(OH)(2-2x)(CO3)(x) (.) yH(2)O (M = Mn, Zn) and 4,4'-bipyridine (bpy) with succinic acid (H2L) or famaric acid (H2L') in CH3OH-H2O afforded [Mn(H2O)(4)(bpy)]L (.) 4H(2)O, 1, [Mn(H2O)(4)(bpy)]L' (.) 4H(2)O, 2 and [Zn(H2O)(4)(bpy)]L (.) 4H(2)O, 3. The three coordination polymers are isostructural and consist of (1)(infinity)[M(H2O)(4)(bpy)(2/2)](2+) cationic chains, crystal H2O molecules and dicarboxylate anions (succinate or fumarate anions). Within the chains, the metal atoms are each octahedrally coordinated by four aqua oxygen atoms and two pyridyl nitrogen atoms from two 4,4'-bipyridine ligands. The crystal H2O molecules are hydrogen bonded to dicarboxylate anions to form ribbon-like anionic chains. The cationic and anionic chains are interconnected via hyqrogen bonds to generate a 3D network. Crystal data: 1 triclinic, P (1) over bar, a = 7.235(1), b = 7.749(2), c = 10.020(2) Angstrom, alpha = 79.95(3), beta = 88.79(3), gamma = 71.39(3)degrees, V = 523.9(2) Angstrom(3) and D-cal = 1.494 g cm(-3) for Z = 1; 2 triclinic, P (1) over bar, a = 7.127(1), b = 7.800(2), c = 9.945(2) Angstrom, alpha = 80.26(3), beta = 87.86(3), gamma = 72.69(3)degrees, V = 520.2(2) Angstrom(3) and D-cal = 1.498 g cm(-3) for Z = 1; 3 triclinic, P (1) over bar, a = 7.189(1), b = 7.764(2), c = 9.843(2) Angstrom, alpha = 79.16(3), beta = 87.80(3), gamma = 71.29(3)degrees, V = 510.9(2) Angstrom(3) and D-cal = 1.559 g cm(-3) for Z = 1.

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A new photoluminescent heterobimetallic Zn(II)-Ag(I) cyano-bridged coordination polymer, [Ag5Zn2(tren)(2)(CN)(9)] (tren = tris(2-aminoethyl)amine) (1), has been synthesized and structurally characterized. It features rare linear pentameric unit of dicyanoargentate(I) ions assembled by d(10)-d(10) interaction as building blocks. Solid state emission spectrum of I shows strong ultraviolet luminescence with emission peak in the range of 376 nm.

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近年来,有机薄膜晶体管(OTFTs)因其成本低、加工简便,特别适用于制备大面积柔性器件而引起人们的广泛关注[1].并苯类化合物和噻吩衍生物是目前最重要的两类高迁移率OTFT材料.由并五苯制备的多晶OTFTs器件迁移率可达到5cm2/(V·s)[2];烷基修饰齐聚噻吩的场致迁移率也可达到非晶硅[0·1~1cm2/(V·s)]的水平[3].但是,这两类材料具有较窄的能隙和较高的最高被占分子轨道(HOMO)能级,容易与空气中的氧气和水发生作用,所制备的器件在空气中衰减较快,并且并苯类化合物对光也非常敏感,限制了其应用范围[4~6].因此,制备稳定的高迁移率有机半导体材料是有机光电子研究领域的重要课题之一.制备稳定的高迁移率有机半导体材料的途径包括用较稳定的芳香基团对噻吩齐聚物进行封端,以增大能隙和降低HOMO能级[7].菲类化合物是并苯类化合物的异构体,具有较好的光稳定性[8].[3,2-b]并二噻吩是一种平面稠环分子,与2,2′-二噻吩相比,HOMO能级相对降低,因而具有相对好的稳定性[9].本文合成了2,5-二(2-菲基)-[3,2-b]并二噻吩(PhTT),表征了其基本的物理和化学性质,制备了相应的有机薄膜晶...