557 resultados para Bad Laer Z 1


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The Hamiltonian of the wurtzite quantum rods with an ellipsoidal boundary is given after a coordinate transformation. The energies, wave functions, and transition possibilities are obtained as functions of the aspect ratio e with the same method we used on spherical dots. With an overall consideration of both the transition matrix element and the Boltzmann distribution we explained why the polarization factor increases with increasing e and approaches a saturation value, which tallies quite well with the experimental result. When e increases more and more S-z states are mixed into the ground, second, and third states of J(z)=1/2, resulting in an increase of the emission of z polarization. It is just the linear terms of the momentum operator in the hole Hamiltonian that cause the mixing of S and P states in the hole ground state. The effects of the crystal field splitting energy, temperature, and transverse radius to the polarization are also considered. We also calculated the band gap variation with the size and shape of the quantum rods.

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I LnCl_3-LiCl-THF配合物的研究深入地研究了氯化稀土和氯化锂于四氢呋喃溶液中,以不同的摩尔比,在不同条件下的反应。实验结果表明,反应速度随着稀土元素原子半径的减小,LiCl/LnCl_3摩尔比的增大,以及四氢呋喃用量的增加而加快。通过紫外质谱元素分析和X-射线单晶结构分析等证明,随着不同的LiCl/LnCl_3摩尔比和结晶条件的不同,可以得到不同组成的LnCl_3-LiCl-TNF配合物。对(LaCl)(THF)_2(μ_2-Cl)_4[Li(THF)_2]_2和(LaCl)DME(μ_3-Cl)(μ_2-Cl)_5(La·DME)Li(THF)_2晶体的结构分析表明,前者为单斜晶系,P21/C空间群。a=10.542(4), b=32.236(4), c=11.182(6)A °; β=113.50(3) °, V=3484.97 A °~3. Z=4, R=0.0471;后者为三斜晶系,PT空间群,晶胞参数是:a=11.123(3), b=16.564(5), c=8.653(3)A °;α=95.16(3), β=95.63(3), γ=74.71(3) °;V=1527.0A °~3。Z=2,R=0.0303。实验结果还表明,μ_2-和μ_3-氯桥键是LnCl_3-LiCl-THF类配合物中最基本、最重要的配位键,这种键是通过多重键的方式起着稳定分子结构的作用。当进行与有机配体的交换反应时,由于它们的特殊稳定性,能起到阻止轻稀土有机配合物歧化反应的作用。II环戊二烯基轻镧系氯化物的合成及其稳定性的研究对(G_5H_5)_3Ln·THF和LnCl_3·3LiCl-THF (Ln=La, Nd)溶液反应的研究表明,由于μ_2-氯桥键的作用,轻稀土环戊二烯基化合物中环戊二烯基的再分配反应,在0℃或室温下都能迅速进行。通过两者不同的摩尔比反应,经元素分析、红外光谱、~1H NMR和质谱鉴定,方便地合成了C_5H_5 LnCl_2·2LiCl·5THF和(C_5H_5)_2LnCl.LiCl·nTHF (Ln=La, Nd)等配合物。这一结果表明(C_5H_5)_2LnCl.LiCl·nTHF配合物不仅能稳定地存在于THF溶液中,而且能在一定条件下析出结晶。对(C_5H_5)_2LaCl.LiCl·4THF的晶体结构测定表明,该晶体属于正交晶系,Pc2m空间群。a=12.306(4), b=23.056(6), c=26.701(11)A°; V=7575.81A°~3;而(C_5H_5)_2LaCl·LiCl(DME)_2THF晶体则属于六方晶系,a=12.967(4), b=12.967(4), c=24.108(10)A°;V=3510 A°~3。通过(G_5H_5)_3Ln·THF与LnCl_3·3THF (Ln=La, Nd)的反应进一步研究了轻稀土环戊二烯基氯化物的稳定性。经元素分析,红外光谱和晶体结构分析表明合成了[(η~5-C_5H_5)_4La_3Cl_5·3THF]_2·9THF和(C_5H_5)_2 NdCl·THF配合物,前者属于三斜晶系,P1空间群。a=11.690(3), b=11.750(5), c=18.433(6)A°; α=98.75(3), β=95.62(3), γ=118.92(2)°; V=2147.06 A°~3. Z=1, R=0.099。对环戊二烯基轻稀土氯化物的稳定性进行了较详细地讨论。结果表明,THF的用量和化合物的溶解度是影响产物组成的决定因素。当THF的量不足以溶解所生成的产物时,就会歧化成溶解度最大((C_5H_5)_3Ln·THF)和最小(LnCl_3·nTHF)的两种组分。反之,环戊二烯基轻稀土化合物(Ln=La, Nd)中环戊二烯基的再分配反应就能顺利进行。经元素分析和结构测定,在((C_5H_5)_3Nd·THF)和NdCl_3·LiCl-THF溶液的反应体系中,偶然分离得到了[(η~5-C_5H_5)_4Nd_4(μ_4-o)(μ_2-Cl)_8] [Li(DMP)_2THF]_2这一不合常规的化合物,其晶体属于正交晶系,Pna2,空间群a=19.010(7), b=23.231(6), c=14.180(4); V=6261.91 A°~3。Z=4, R=0.054。说明在一定条件下,μ-氧桥键也起到了稳定分子结构的作用。推测了各类环戊二烯基轻稀土氯化物在THF中的合成反应机理,在LiCl存在的反应体系中Ln cl cl Li桥键能与环戊二烯基发生交换反应;在(C_5H_5)_3Ln·THF和LnCl_3·3THF的反应体系中,首先存在着LnCl_3分子之间的互相作用,因而易于形成双核或多核配合物。这类配合物以晶体形式析出时,易于发生结构上的变化,即化合物的结晶形态与溶液中的形态不一定相同。探索了环戊二烯基烯丙基稀土化合物新的合成方法。找到了真空加热脱水制备氯化稀土的最佳条件,其产物纯度在97%以上。通过加入Co_3O_4/Wo_3催化助燃剂的方法,提高了测定稀土有机化合物中碳含量的准确性。

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In this study, the energy for the ground state of helium and a few helium-like ions (Z=1-6) is computed variationally by using a Hylleraas-like wavefunction. A four-parameters wavefunction, satisfying boundary conditions for coalescence points, is combined with a Hylleraas-like basis set which explicitly incorporates r12 interelectronic distance. The main contribution of this work is the introduction of modified correlation terms leading to the definition of integral transforms which provide the calculation of expectation value of energy to be done analytically over single-particle coordinates instead of Hylleraas coordinates.

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采用射频磁控反应溅射技术与热退火处理制备了Si/SiN;超晶格材料。利用吸收光谱和X射线衍射对材料进行表征。通过皮秒脉冲激光单光束Z-扫描技术研究了该材料在非共振吸收区的三阶非线性光学特性,实验结果表明,样品的非线性折射率为负值,非线性吸收属于双光子吸收。由实验数据得到材料的三阶非线性极化率实部和虚部分别为1.27×10~(-7),1.51×10~(-8)esu,该值比体硅材料的三阶非线性极化率值大5个数量级。对材料光学非线性产生的机理进行了探讨,认为材料的非线性极化率的增加来源于材料量子限制效应的增强。

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Planar punch through heterojunction phototransistors with a novel emitter control electrode and ion- implanted isolation (CE-PTHPT) are investigated. The phototransistors have a working voltage of 3-10V and high sensitivity at low input power. The base of the transistor is completely depleted under operating condition. Base current is zero. The CE-PTHPT has an increased speed and a decreased noise. The novel CE-PTHPT has been fabricated in this paper. The optical gain of GaAlAs/GaAs CE-PTHPT for the incident light power 1.3 and 43nw with the wavelength of 0.8 mu m reached 1260 and 8108. The input noise current calculated is 5.46 x 10(-16) A/H-z(1/2). For polysilicon emitter CE-PTHPT, the optical gain is 3083 at the input power of 0.174 mu w. The optical gain of InGaAs/InP CE-PTHPT reaches 350 for an incident power of 0.3 mu w at the wavelength of 1.55 mu m. The CE-PTHPT detectors is promising as photo detectors for optical fiber communication system.

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干扰素(IFNs)是最早发现的具有广泛用途的一类细胞因子,IFN-α通过JAK/STAT信号途径调控机体一系列生理和病理反应。至今尚未发现类干扰素的小分子。我们前期研究发现天然产物毛蕊异黄酮可激活干扰素诱导的JAK/STAT信号途径。为发现类干扰素小分子、获得小分子探针,本课题拟建立成熟的JAK/STAT信号途径的筛选模型,合成毛蕊异黄酮及其类似物,研究这些化合物的构效关系,进而尝试通过共价键标记生物素或香豆素来直接研究它们与相关受体的作用。 从异香草醛出发经7步合成反应得到了毛蕊异黄酮。采用平行合成策略得到异黄酮类化合物;采用分支式合成策略,以取代苯乙酸作为合成砌块,获得具有与异黄酮类似结构的香豆素、3-芳基喹诺酮。与分离得到的黄酮类化合物,构建了一个包括异黄酮、黄酮、香豆素、3-芳基喹诺酮在内的化合物库。 建立了包含IFN-α刺激反应元件 (ISRE)的荧光素酶报告基因体系,通过筛选化合物库中的化合物,发现异黄酮骨架为激活JAK/STAT信号途径必须结构、毛蕊异黄酮7-位酚羟基被取代后活性丧失。根据以上结果,对毛蕊异黄酮3′-位标记物的合成进行了初步尝试。 发现山茱萸科植物青荚叶(Helwingia japonica (Thunb.) Dietr.)有抑制蛋白酪氨酸磷酸酯酶1B(PTP1B)的活性。从其地上部分95%乙醇提取物的乙酸乙酯部分分离得到5个化合物,应用波谱方法及与已知品对照的手段鉴定它们为p-menth-2-en-1β, 4β, 8-triol (Z-1)、blumenol A (Z-2)、2′,3′,4′,5′,6′-五羟基查尔酮(Z-3)、洋芹素7-O-β-D-吡喃葡萄糖苷(Z-4)、木犀草素7-O-β-D-吡喃葡萄糖苷(Z-5). Interferons (IFNs) are one kind of cytokines with broad functions. IFN-α mediates series physiological and pathological changes of human body via JAK/STAT pathway. Untill now, no IFNs-like small molecules are discovered. In our preliminary experiment, the natural product calycosin has been observed to activate JAK/STAT pathway. Therefore, we establish a luciferase reporter gene system and synthesize calycosin and its analogues to reveal their structure-activity relationship (SAR). Besides, in order to prove that calycosin activates JAK/STAT pathway through IFN receptor, we attempted to tag it with biotin or coumarin by covalent bonding. Calycosin was synthesized from isovanillin via seven steps. Other isoflavones were obtained by parallel synthesis; coumarins and quinolones were prepared through divergent synthesis, using substituted phenylacetic acids as building blocks. Combing with natural flavones, a small molecule library was established. A luciferase reporter gene system, consisting of 5 copies of the ISRE (interferon-stimulated response element), was used for screening of small molecules from that library. We found that the core-structure of isoflavone was necessary, and if the 7-OH is substituted, the activity slumps. According to our observation, we tried to tag biotin or coumarin at 3′-OH of calycosin. The 95% ethanol extract of the aerial parts of Helwingia japonica (Thunb.) Dietr. showed protein tyrosine phosphatase 1B (PTP1B) inhibitory activity. Five compounds were isolated. On the basis of spectral data or by comparison with authentic samples, they were identified as p-menth-2-en-1β,4β,8-triol (1), blumenol A (2), 2′,3′,4′,5′,6′-pentahydroxychalcone (3), apigenin 7-O-β-D-glucopyranoside (4), and luteolin 7-O-β-D-glucopyranoside (5).

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综述了自提出冷熔合反应作为合成原子序数 Z>1 0 6号超重元素的最主要反应机制以来 ,冷熔合合成超重元素所取得的重大成就及其进展至目前所面临的困惑 .详细介绍了最近国际上围绕 1 1 8号元素合成以及对以冷熔合反应合成 Z>1 1 2号超重元素前景上的争论 .讨论了在我国现有实验条件下 ,基于冷熔合机制开展超重元素合成面临的问题

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放射性束流(RIB)装置拓广了实验核物理在同位旋(T_z)自由度上从稳定核直到滴线核的广袤空间。通常,位于β-稳定线及其附近的核,N/Z11.5范围变化,其分离能E_s无论对于质子还是中子,总是在6-8 MeV之间;对于远离稳定线的非稳定核,N/Z可在0.5-4范围变化,如~9C的N/Z = 0.5,~(10)He的N/Z = 4,而且分离能E_s是在0-40 MeV之间变化的,开展对这些远离β-稳定线非稳定核性质、结构的研究是目前核物理的前沿之一。核反应总截面σ_R是表征原子核性质特征的一个基本物理量,从实验测得的核反应总截面中可以得到有关核结构和核内核子分布的信息。在由放射性束流所产生奇异核的结构与各种反应机制研究中,反应总截面的测量更是有其特殊的重要性,具有奇异核结构如晕核的一个典型的物理特征就是其反应总截面要比稳定核大得多,Tanihata等人最早就是通过对放射性束流的相互作用截面的测量发现了具有奇异结构的核,即中子晕核。由于反应总截面的测量对探测器的要求不高,而且数据分析过程相对较为简单,因而反应总截面的测量已经成为放射性束核物理的研究的一个非常重要实验手段。中子晕核以及中子皮核的发现促使人们去寻找质子晕核和质子皮核,由于最后一个质子的结合能非常小只有136,keV,并且有较大的电四极矩,因而使得~8B成为质子晕的最大热门候选核,有关~8B是否具有质子晕核结构的问题,许多实验科学家得出了相互矛盾的回答;而目前有关另外一个质子晕候选核~9C的实验数据非常少,目前还没有人从实验上对~9C是否为质子晕核这一问题进行肯定或否定的回答。因此非常有必要测量~9C和~8B的反应总截面。对反应总截面进行研究的一个非常有用理论就是Glauber模型,该模型考虑了库伦效应的多次散射理论。它是一种基于自由核子-核子(N-N)碰撞的与核物质密度相关的理论,因而能够从实验测量到的反应总截面中提取核物质分布的信息。该理论对中低能区的反应总截面描述却有一个缺憾:理论值比实验值都要小。本论文主要描述了利用透射法测量了中能区同中子素核~9C、~8B、~7Be及~6Li与~(28)Si的反应总截面,并介绍了重离子碰撞以及描述重离子性质的几种常用理论。在论文里对实验测量得到的结果进行了理论分析,这些理论包括半经验的Shen公式、Glauber模型、BUU模型以及SHF理论。如果将~9C和~8B当成具有正常核结构来处理,半经验的Shen公式和Glauber模型(HO密度分布)的理论计算值总是比实验值要小得多;对于Glauber模型的理论计算值和实验值的差异,Ozawa等定义了一个差值因子d,方德清等人对轻核系统的d值进行了详细的分析。一般认为,正常核的d值在20%以内,而对于具有晕或皮奇异结构的核,其d值则超过30%,甚至可达50%,因此可根据一个核的d值是否超过30%而且比相邻核的d值明显大这种半经验的方法来判断一个核是否具有奇异结构;利用d值的分析结果,我们认为:~9C和~8B都具有奇异核结构;对于BUU模型用同样的方法引进差值因子d值,对于~9C和~8B有相同的结论。用SHF理论计算得到B和C同位素的密度分布结果显示,~9C和~8B的密度分布比相邻的同位素扩展都要大得多。为减小Glauber模型计算的反应截面与实验值的差别,本论文还对Glauber模型的输入密度形式进行了修改,在原单一HO分布基础上加一个高斯分布的尾巴,并对丰质子的同中子素核~9C、~8B、~7Be及~6Li与~(28)Si靶以及~(12)C和丰中子的C同位素核~(13-16)C与~(12)C靶的反应截面重新进行了计算,结果显示在中能区的计算值比原来单一密度分布的计算结构有明显改善。

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中能重离子碰撞中的核反应机制及其形成的高激发热核的性质是中能重离子物理研究的重要领域,而高激发热核性质的同位旋效应研究是这一领域的热点之一。选取了具有不同N亿比的反应体系以研究激发热核性质的同位旋效应。本论文涉及的反应系统三对共六个反应体系:55MeV/u~(40)Ar+~(58.64)Ni、30MeV/u~(40)Ar+~(112,124)Sn、35Mev/u~(36)Ar+~(112,124)Sn,这六个反应体系的N/z比分别为1.13,1.26、1.24,1.411.18,1.35。分别从带电粒子多重性、相对态布居核温度、关联函数等角度研究了这三对反应体系高激发热核性质的同位旋效应。在55MeV/u 40Ar+58,64Ni核反应中,用兰州4π带电粒子探测器阵列测量带电粒子多重性,研究了He和中等质量碎片的产额与反应系统的同位旋的关系,以及这种同位旋效应与反应系统的碰撞参数(即碰撞的激烈程度)、系统的激发能的变化关系。对两个反应系统,观察到带电粒子多重性中He的比分随带电粒子多重性的增加而增大,带电粒子多重性中IMF的比分随带电粒子多重性的增加而先增大,后减小的规律。两个反应系统虽然具有相同的核电荷数,但轻粒子He和中等质量碎片在多重性中的比分有明显的同位旋相关性。在30Mev/u40Sn、35MeV/u~(40)Ar~(112,124)Sn、35Mev/u 36Ar+112,124Sn反应中用13单元望远镜探测器阵列测量了小角关联粒子。由价a关联函数提取了30Mev/u 40Ar+112,12Sn反应系统中激发热核的态布居核温。对于不同同位旋反应系统舜UAr+112Sn和4VAr+124Sn,提取的相对杰布居核温度分别是4.18+0.28/0.21MEV和4.10士0.22/0.20MeV;考察态布居核温度和粒子能量的关薰时,观察到两个系统的发射温度均随着粒子能量的增加而降低,缺中子系统40Ar+l12Sn中由低能时的5.13士.30/0.26MEV降低到高能时的3.87士0.37/0.29MeV,丰中子系统40Ar+124Sn中由低能时的5.39士0.30/0.26MeV降低到高能时的3.32士MeV。讨论了这种布居态核温度的同位旋相关性。在35Mev/u 36Ar+112,124Sn反应中提取了洲F(3‘25)的约化速度关联函数。相对丰中子36Ar+124Sn系统的IMF关联函数在小约化速度处反关联程度更强,表明36Ai+124Sn系统的发射IMF的平均时间更短。用MENEKA程序提取了两个系统IMF的平均发射时间,36Ai+112sn反应中IMF的发射时间约为150fm/c,而36Ar十124Sn反应IME的发射时间稍短,约为120fm/c。以关联IMF的单核子总能量/动量为窗条件,发现低能IMF关联函数几乎没有差别,而高能IMF关联函数在小约化速度处的差别更为明显,表明两个系统IMF关联函数的同位旋效应可能来自于IMF的早期发射。为了得到进一步的信息,我们提取了高动量窗条件下的IMF发射时间,它们比平均发射时间短,36Ar+112Sn反应中高能IMF的发射时间约为100蒯c,而36Ai+124Sn反应中IMF的发射时间则更短,约为50fm/c。

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位置灵敏Bragg探测器的研制,是为实现戴光曦老师提出的设想:在Bragg探测器的内部实现对位置测量而进行的一项研究工作。这项工作的实现对中、低能重离子核反应完成对裂片的测量是很有意义的。本工作采用电阻串进行电荷分除来定位,这在近物所为第一次。试验中,同时测量位置,能量及电荷对~(252)C+源的α粒子可以达到:ΔE/E = 1.9%, ΔZ/Z = 1.6% ΔX好于9mm

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重离子核反应机制的研究一直是人们关注的课题。用25MeV/u 40Ar的束流进行多种反应机制共存及其对碎片的贡献的研究,有助于我们更清楚地了解反应机制的演化和对放射性束流产额的预言。 实验中用25MeV/u40Ar的束流轰击115In、58Ni、27Al,这时对前方向6°、8.5°的碎片测量,发现它们的平行动量分布宽度满足Goldhaber关系式,碎裂部分提取的约化平行动量分布宽度σ0=54MeV/c,这比弹核碎裂部分的宽度要窄,说明转移反应比弹核碎裂受到相空间的严格限制更严格。转移反应主要是对弹核附近的碎片有贡献,当类弹碎片质量与弹核质量相差较大时,主要是弹核碎裂的贡献。对于弹核碎裂产物的最可几能量的提取,在实验能谱中拟合出碎片的最可几能量,对于接近弹核的碎片,我们利用外推法来确定碎裂部分的最可几能量,同时用实验提取的σ0值,拟合出碎裂能谱,从而将弹核碎裂和转移反应的贡献区分开来。 通过碎片同位素的测量,我们认碎片的同位素分布与靶核有一定的依赖关系,当靶核的N/Z值增加时,产物的N/Z也增加。弹核40Ar的N/Z1.22,靶核的N/Z均大于1,所以产物N/Z的变化意味着系统由非平衡向平衡的演化,且在这一能区,重离子反应既有低能下一体耗散的特点,又有高能下核子-核子碰撞的特点,多种反应机制共存并竞争。

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A new polyoxometalate [Co(phen)(3)](2)[HPMo4V Mo-4(VI) V-6(IV) M2O44]center dot 4H(2)O (M = 0.78Mo(V)+ 0.22V(IV)) 1 was hydrothermally synthesized and characterized by IR, elemental analyses, X-ray photoelectron spectrum, ESR and single crystal X-ray diffraction. The title compound is in the triclinic space group P (1) over bar with a = 12.0953(7) angstrom, b = 14.0182(6) angstrom, c = 14.6468(7) angstrom, V=2402.55(18) angstrom(3), alpha = 105.134(2), beta = 91.841(3), gamma = 91.401(2), Z = 1, and R-1 (wR(2)) = 0.0617 (0.1701). The compound was prepared from tetra-capped pseudo-Kepin with phosphorus-centered polyoxoanions [PMo8V6M2O44](5-) , [Co(phen)(3)](2+) cations and linked through hydrogen bonds and pi-pi stacking interaction into three-dimensional supramolecular framework. Astudy of the magnetic properties of 1 demonstrates that it exhibits antiferromagnetic coupling interactions.

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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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The hydrothermal reactions of vanadium oxide starting materials with divalent transition metal cations in the presence of nitrogen donor chelating ligands yield the bimetallic cluster complexes with the formulae [{Cd(phen(2))(2)V4O12].5H(2)O (1) and [Ni(phen)(3)](2)[V4O12] . 17.5H(2)O (2). Crystal data: C48H52Cd2N8O22V4 (1), triclinic. P (1) over bar, a = 10.3366(10), b = 11.320(3), c = 13.268(3) Angstrom, alpha = 103.888(17)degrees, beta = 92.256(15)degrees, gamma = 107.444(14)degrees, Z = 1; C72H131N12Ni2O29.5V4 (2), triclinic. P (1) over bar, a = 12.305(3), b = 13.172(6), c = 15.133(4), alpha = 79.05(3)degrees, beta = 76.09(2)degrees, gamma = 74.66(3)degrees, Z = 1. Data were collected on a Siemens P4 four-circle diffractometer at 293 K in the range 1.59degrees < theta < 26.02degrees and 2.01degrees < 0 < 25.01degrees using the omega-scan technique, respectively. The structure of 1 consists of a [V4O12](4-) cluster covalently attached to two {Cd(phen)(2)}(2+) fragments, in which the [V4O12](4-) cluster adopts a chair-like configuration. In the structure of 2, the [V4O12](4-) cluster is isolated. And the complex formed a layer structure via hydrogen bonds between the V4O12](4-) unit and crystallization water molecules.

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A new compound, (CH5N2)(3)(PMo12O40CH4N23H2O)-C-.-H-. (1), was synthesized and structurally characterized by elemental analyses, IR spectra, UV spectra, NMR spectra and ESR spectra. This is, to our knowledge, the first example of an imidazole-polyoxometalate species. The compound was recrystallized from N,N-dimethylformamide (DMF), and then black block-like crystals of (C3H5N2)(4)((PMoMo11O40)-Mo-V-O-VI)(.)4C(3)H(7)NO(.) 2H(2)O (2), were obtained. It crystallizes in a triclinic space group P (1) over bar with n=12.423(3) Angstrom, b=12.666(3) Angstrom, c=13.341(3) Angstrom, alpha=70.56(3)degrees, beta=71.16(3)degrees, gamma=64.18(3)degrees, V= 1742.3(6) Angstrom(3), Z=1, R1 = 0.0585, wR2 = 0.1885. An X-ray crystallographic study showed that the crystal structure is constructed by electrostatic attractions and hydrogen bonds between a dodecamolybdophosphoric anion and an imidazole. The imidazole and DMF molecules occupy cavities in a polyoxometalate lattice ordered along a c-axis. The structure of (2) is similar to that of (1) from a comparison of both IR spectra and TGA Curves.