[Nd(4-PYA)_3(H_2O)_2]_n的合成及其晶体结构

3-(4-吡啶基)丙烯酸(4-HPYA)和Nd(NO3)3通过水热法合成了一种新的一维链状配位聚合物[Nd(4-PYA)3(H2O)2]n(1),其结构经IR,元素分析和X-射线单晶衍射表征。1属三斜晶系,P-1空间群,晶胞参数:a=0.829 23(13)nm,b=1.272 60(2)nm,c=1.435 00(12)nm,α=112.371(2)°,β=98.856(3)°,γ=100.239(2)°,V=1.336 6(3)nm3,Mr=660.72,Z=2,Dc=1.642 g.cm-3,F(000)=662,μ=2.002mm-1,R1=0.052 3,wR2=0.141 9。1通过分子间氢键作用将一维链紧密堆积成三维网状结构。     

[(C_6H_5NO_2)Pr(H_2O)_4](CrMo_6O_(24)H_6)·(C_6H_5NO_2)·2.5H_2O的合成与晶体结构

用常规合成方法制备了基于Anderson结构阴离子的二维层状化合物[(C6H5NO2)2Pr(H2O)4](CrMo6O24H6)·2.5H2O,通过红外光谱和X射线单晶衍射对其进行了表征.结果表明,该化合物属于单斜晶系,C2/c空间群.a=2.3442(9)nm,b=1.3291(5)nm,c=2.458(1)nm,β=103.08(1)°,V=7.460(5)nm3,R1=0.0727,wR2=0.1903.结构分析表明,[CrMo6O24H6]3-阴离子通过端氧担载一个配位的Pr3+离子形成中性的(C6H5NO2)Pr(H2O)4(CrMo6O24H6)基团,相邻的中性基团在Ot—Pr—Ot桥联下形成一维链,链与链又通过异烟酸的桥联形成二维层状结构.     

[（C6n5NO2）Pr（H2O）4]（CrMo6O24H6）·（C6H5NO2）·2．5H2O的合成与晶体结构

用常规合成方法制备了基于Anderson结构阴离子的二维层状化合物[（C6n5NO2）Pr（H2O）4]（CrMo6O24H6）·（C6H5NO2）·2．5H2O,通过红外光谱和X射线单晶衍射对其进行了表征．结果表明,该化合物属于单斜晶系,C2/c空间群．a=2．3442（9）nm,b=1．3291（5）nm,c=2．458（1）nm,β=103．08（1）°,V=7．460（5）nm^3,R1=0．0727,wR2=0．1903．结构分析表明,[CrMo6O24H6]^3-阴离子通过端氧担载一个配位的Pr^3＋离子形成中性的（C6H5NO2）Pr（H2O）4（CrMo6O24H6）基团,相邻的中性基团在O1-Pr-O1桥联下形成一维链,链与链又通过异烟酸的桥联形成二维层状结构．     

1,3-二(4-吡啶基)丙烷Cd(Ⅱ)配合物的合成、晶体结构及发光性质研究

以1,3-二(4-吡啶基)丙烷(L)为配体,合成了一种新的Cd(Ⅱ)配合物{[CdL2(H2O)2].2(C7H6N5)}n(C7H6N5=5-(3-氨基苯基)四唑离子)。X射线单晶衍射结构分析表明该配合物为一维链状结构,Cd(Ⅱ)分别与4个1,3-二(4-吡啶基)丙烷配体的4个氮原子,2个配位水分子的氧原子形成了六配位的扭曲八面体几何构型,1,3-二(4-吡啶基)丙烷配体桥梁相邻的Cd(Ⅱ)离子形成了一维的无限延伸的链状结构,分子间通过O-H…N、N-H…N氢键作用构筑成三维超分子网络结构。     

具有三维网络的新型配位聚合物[Nd(C7H6NO2)3.H2O]n的合成、结构和性质

以Nd(NO3).6H2O和NH2C6H4COOH为原料,经[Nd(C7H6NO2)3.H2O]的自组装,得到了具有三维网络结构的配位聚合物[Nd(C7H6NO2)3.H2O]n。该聚合物晶体属单斜晶系,空间群P2(1)/n,a=0.98069(5)nm,b=2.2736(2)nm,c=0.98254(8)nm,β=100.053(5)°,V=2.1571(3)nm^3,Z=4。最后的一致性因子R=0.038。磁性研究表明,该化合物在低温下表现出反铁磁性质。测定了化合物的UV-vis-NIR和IR光谱,进行了分析和指认。     

[（C6n5NO2）Pr（H2O）4]（CrMo6O24H6）·（C6H5NO2）·2．5H2O的合成与晶体结构

用常规合成方法制备了基于Anderson结构阴离子的二维层状化合物[（C6n5NO2）Pr（H2O）4]（CrMo6O24H6）·（C6H5NO2）·2．5H2O,通过红外光谱和X射线单晶衍射对其进行了表征．结果表明,该化合物属于单斜晶系,C2/c空间群．a=2．3442（9）nm,b=1．3291（5）nm,c=2．458（1）nm,β=103．08（1）°,V=7．460（5）nm^3,R1=0．0727,wR2=0．1903．结构分析表明,[CrMo6O24H6]^3-阴离子通过端氧担载一个配位的Pr^3＋离子形成中性的（C6H5NO2）Pr（H2O）4（CrMo6O24H6）基团,相邻的中性基团在O1-Pr-O1桥联下形成一维链,链与链又通过异烟酸的桥联形成二维层状结构．     

具有三维网络的新型配位聚合物[Nd(C7H6NO2)32·H2O]n 的合成、结构和性质

以Nd(NO3)3@6H2O和NH2C6H4COOH为原料,经[Nd(C7N6O2)3@H2O]的自组装,得到了具有三维网络结构的配位聚合物[Nd(C7H6NO2)3@H2O]n.该聚合物晶体属单斜晶系,空间群P2(1)/n,a=0.98069(5)nm,b=2.2736(2)nm,c=0.98254(8)nm,β=100.053(5)°,V=2.1571(3)nm3,Z=4.最后的一致性因子R=0.038.磁性研究表明,该化合物在低温下表现出反铁磁性质.测定了化合物的UV-vis-NIR和IR光谱,并进行了分析和指认.     

配合物Nd(C7H7N2O2)3(H2O)3的合成及其晶体结构

用水热法合成了3,5-二氨基苯甲酸与Nd(Ⅲ)的配合物Nd(C7H7N2O2)3(H2O)3(1),其结构经IR,元素分析和X-射线单晶衍射仪表征。1为单核结构,属六方晶系,R3空间群,晶胞参数:a=1.887 29(18)nm,b=1.887 29(18)nm,c=0.603 53(12)nm,β=90,°γ=120°,V=1.861 7(4)nm3,Z=3,μ=2.154 mm-1,Dc=1.744 g.cm-3,R1=0.014 3,wR2=0.033 2。1中Nd(Ⅲ)与来自3个3,5-二氨基苯甲酸的6个氧原子及3个配位水的氧原子进行配位,形成9配位化合物。     

1-D链状簇合物[Ni(enMe)_2]_2[Ni(enMe)_2{HMoo_4~(VI)Mo_4~V_8~(VI)VO_(40)(V~VO_4)}]·4H_2O的水热合成和晶体结构

水热合成了一种新的1-D链状四帽pseudo-Keggin 结构钼钒簇合物[Ni(enMe)2]2- [Ni(enMe)2{H MoVI4MoV4VIV8O40(VVO4)}]4H2O 1,X-射线单晶结构分析表明,该晶体属单斜晶系,C2/c空间群。晶体学参数为a = 26.3006(6), b = 13.6195(3), c = 19.7122(5) ,b = 105.8330(10), V = 6793.0(3) ?, Z = 4, Dc = 2.566 g/cm3, Mr = 2623.96, m = 3.507 mm-1, F(000) =5088, R = 0.0700, wR = 0.1529, S = 1.019。该簇合物是由金属配位桥Ni(enMe)2桥联四帽pseudo-Keggin 结构{HMoVI4MoV4VIV8O40(VVO4)}簇构成一维链状结构,链与链间通过与另外一个配位阳离子[Ni(enMe)2]2+的氢键相互作用构成超分子网状结构。     

新型一维配位聚合物{[Cu(H2L)(HL)](ClO4)·3H2O}n的合成及其晶体结构

Cu(ClO4)2·6H2O与H2L{L=[2,3-f]-吡嗪[1,10]邻菲咯啉-2,3-二甲酸}反应合成了新型一维配位聚合物{ [Cu(H2L) (HL)] (C1O4)· 3H2O}n(1),其结构经UV,IR,XRD和元素分析表征. 1属单斜晶系,空间群C2/c,晶胞参数a=3.575 9(13) nm,b=0.962 7(3)nm,c=2.127 5(10)nm,β=116.106(8)°,V=6.577(5) nm3,Z=8,Dc=1.730 g·cm-3,Mr=856.56,F(000)=3 480,μ=0.837nm-1,R=0.082 6,wR=0.248.Cu2+分别与1个H2L的两个氮原子,2个不同μ2-HL的两个氮原子和一个羧酸氧原子配位,形成畸变四方锥的五配位构型.Cu(Ⅱ)通过HL桥联形成一维链,相邻一维链的芳环π-π堆积和分子间氢键作用使1构筑成三维超分子结构.     

The bivalent metal hypophosphites Sr(H2PO2)2, Pb(H2PO2)2 and Ba(H2PO2)2

The structures of isomorphous monoclinic strontium and lead bis­(di­hydrogenphosphate), Sr(H₂PO₂)₂ and Pb(H₂PO₂)₂, and orthorhombic barium bis­(di­hydrogen­phos­phate), Ba(H₂PO₂)₂, consist of layers of hypophosphite anions and metal cations exhibiting square antiprismatic coordination by O atoms. The Sr and Pb atoms are located on sites with point symmetry 2, and the Ba atoms are on sites with point symmetry 222. Within the layers, each anion bridges four metal cations.     

Synthesis and Crystal Structures of Two Complexes [Mn2(L)2(H2bta)2(H2O)]n and[Cu2(L)(H2bta)0.5(H2O)]n

Two new complexes, [Mn₂(L)₂(H₂bta)₂(H₂O)]_n ( 1 ) and [Cu₂(L)(H₂bta)_0.5(H₂O)]_n ( 2 ) (H₄bta=1,2,4,5‐benzene‐tetracarboxylic acid, L=imidazo[4,5‐f][1,10]phenathroline) were prepared under hydrothermal conditions and their structures determined by single‐crystal X‐ray diffration. The X‐ray diffraction reveals that complex 1 , consisting of two crystallographically independent fragments A1 and A2, displays an interesting 3D supramolecular network constructed with ABAB sequence through hydrogen bonding interactions. In complex 2 , the copper atoms connected by the H₂bta^2? ligands, the chains also are assembled into a 3D honeycomb configuration network formed by moleculars and aromatic π‐π stacking interactions.     

Ferromagnetism in malonato-bridged copper(II) complexes. Synthesis,crystal structures,and magnetic properties of [[Cu(H2O)3][Cu(mal)2(H2O)]]n and [[Cu(H2O)4]2[Cu(mal)2(H2O)]][Cu(mal)2(H2O)2][[Cu(H2O)4][Cu(mal)2(H2O)2][(H2mal = malonic acid)

Three malonato-bridged copper(II) complexes of the formulas [[Cu(H2O)3][Cu(C3H2O4)2(H2O)]]n (1), [[Cu(H2O)4]2[Cu(C3H2O4)2(H2O)]] [Cu(C3H2O4)2(H2O)2][[Cu(H2O)4][Cu(C3H2O4)2(H2O)2]] (2), and [Cu(H2O)4][Cu(C3H2O4)2(H2O)2] (3) (C3H2O4 = malonate dianion) have been prepared, and the structures of the two former have been solved by X-ray diffraction methods. The structure of compound 3 was already known. Complex 1 crystallizes in the orthorhombic space group Pcab, Z = 8, with unit cell parameters of a = 10.339(1) A, b = 13.222(2) A, and c = 17.394(4) A. Complex 2 crystallizes in the monoclinic space group P2/c, Z = 4, with unit cell parameters of a = 21.100(4) A, b = 21.088(4) A, c = 14.007(2) A, and beta = 115.93(2) degrees. Complex 1 is a chain compound with a regular alternation of aquabis(malonato)copper(II) and triaquacopper(II) units developing along the z axis. The aquabis(malonato)copper(II) unit acts as a bridging ligand through two slightly different trans-carboxylato groups exhibiting an anti-syn coordination mode. The four carboxylate oxygens, in the basal plane, and the one water molecule, in the apical position, describe a distorted square pyramid around Cu1, whereas the same metal surroundings are observed around Cu2 but with three water molecules and one carboxylate oxygen building the equatorial plane and a carboxylate oxygen from another malonato filling the apical site. Complex 2 is made up of discrete mono-, di-, and trinuclear copper(II) complexes of the formulas [Cu(C3H2O4)2(H2O)2]2-, [[Cu(H2O)4] [Cu(C3H2O4)2(H2O)2]], and [[Cu(H2O)4]2[Cu(C3H2O4)2(H2O)]]2+, respectively, which coexist in a single crystal. The copper environment in the mononuclear unit is that of an elongated octahedron with four carboxylate oxygens building the equatorial plane and two water molecules assuming the axial positions. The neutral dinuclear unit contains two types of copper atoms, one that is six-coordinated, as in the mononuclear entity, and another that is distorted square pyramidal with four water molecules building the basal plane and a carboxylate oxygen in the apical position. The overall structure of this dinuclear entity is nearly identical to that of compound 3. Finally, the cationic trimer consists of an aquabis(malonato)copper(II) complex that acts as a bismonodentate ligand through two cis-carboxylato groups (anti-syn coordination mode) toward two tetraaqua-copper(II) terminal units. The environment of the copper atoms is distorted square pyramidal with four carboxylate oxygens (four water molecules) building the basal plane of the central (terminal) copper atom and a water molecule (a carboxylate oxygen) filling the axial position. The magnetic properties of 1-3 have been investigated in the temperature range 1.9-290 K. Overall, ferromagnetic behavior is observed in the three cases: two weak, alternating intrachain ferromagnetic interactions (J = 3.0 cm-1 and alpha J = 1.9 cm-1 with H = -J sigma i[S2i.S2i-1 + alpha S2i.S2i+1]) occur in 1, whereas the magnetic behavior of 2 is the sum of a magnetically isolated spin doublet and ferromagnetically coupled di- (J3 = 1.8 cm-1 from the magnetic study of the model complex 3) and trinuclear (J = 1.2 cm-1 with H = -J (S1.S2 + S1.S3) copper(II) units. The exchange pathway that accounts for the ferromagnetic coupling, through an anti-syn carboxylato bridge, is discussed in the light of the available magneto-structural data.     

An ab initio calculation of the dissociation C2H2(1Σ+) → C2H(2Σ+) + H(2S)

The collinear dissociation of acetylene to C₂H and H is studied by a generalized self-consistent procedure. The dissociation energy, the C-H force constant and stretching frequency are computed.     

Electron energy loss spectroscopy (EELS) of H2O,H2S,H2Se and H2Te

Electronic excitation in H₂O, H₂S, H₂Se and H₂Te molecules has been studied by the EELS technique. Spectra of H₂S and H₂Se are remarkably similar with the 1b₁-nd transition most intense. The intensity of the first transition 1b₁-nsa₁ decreases through H₂O to H₂Se and this transition is absent in H₂Te. Transitions observed by EELS have been compared with optical absorption studies. A correlation diagram of the occupied and the excited states has been provided for these four molecules by making use of UVPES and EELS.     

Proton magnetic shielding in H2O and (H2O)2

The proton magnetic shielding constants in the water molecule and its linear perpendicular dimer are computed from SCF-MO-LCGO wave functions by using the uncoupled Hartree-Fock variation-perturbation procedure due to Karplus and Kolker. The convergence of the calculated shielding constants as well as their gauge dependence is studied. The final results for 17-term polynomial variation function indicate that the best choice for the gauge origin corresponds to the molecular electronic centroid.The calculated proton magnetic shielding constant in the water molecule is in remarkable agreement with experimental data and favourably compares with the best coupled Hartree-Fock results. It follows from the calculations for the water dimer that the H-bond NMR-shift amounts in this case —1.0 ppm and qualitatively agrees with the experimental data for the liquid water.     

Fluxionality of hydrogen ligands in Fe(H)2(H2)(PEtPh2)3

Extensive computational investigations along with additional quasielastic neutron scattering data were used to obtain a consistent picture of the extensive fluxionality of hydride and dihydrogen ligands in Fe(H)(2)(H(2))(PEtPh(2))(3) over a wide range of temperatures from 1.5 to 320 K. We were able to identify three different regimes in the dynamical processes based on activation energies obtained from line spectral broadening. The rotational tunneling lines (coherent exchange of the two hydrogens of the H(2) ligand) are broadened with increasing temperature by incoherent exchange up to about 80 K at which point they merge into a quasielastic spectrum from 100 K to about 225 K. The effective activation energies for the two regions are 0.14 and 0.1 kcal mol(-1), respectively. A third dynamical process with a higher activation energy of 0.44 kcal mol(-1) dominates above 225 K, which we attribute to a quantum dynamical exchange of dihydrogen and hydride ligands. Our detailed density functional theory (DFT) structural calculations involving the three functionals (B3LYP, TPSS, and wB97XD) provide a good account of the experimental structure and rotational barriers when only the hydrogen ligands are relaxed. Full relaxation of the "gas-phase" molecule, however, appears to occur to a greater degree than what is possible in the crystal structure. The classical dihydrogen-hydride exchange path involves a cis-dihydrogen and tetrahydride structure with energies of 6.49 and 7.38 kcal mol(-1), respectively. Experimental observation of this process with much lower energies would seem to suggest involvement of translational tunneling in addition to the rotational tunneling. Dynamics of this type may be presumed to be important in hydrogen spillover from metal particles, and therefore need to be elucidated in an effort to utilize this phenomenon.