二角对称稀土配合物的配位场计算

应用双层点电荷配位场(DSCPCF)模型和不可约张量方法,系统地推导了D_2对称场中f~N(N=1—13)组态各支谱项~(2S+1)L_J(J=0—8和J=1/2—15/2)的配位场微扰矩阵元,讨论了二角场(D_2,G_(2v))中不同配位数(5—12)的DSCPCF参数A_m~k的具体表达式及其在较高对称场(D_4,C_(4v),D_(2d),D_(4d),D_(2h),D_(4h)和O_h)中的约化行为,建立了相应的数学模型,计算程序DSF.D适用于二角、四角及其立方对称场任意配位数的稀土配合物的光谱解析。     

C_(3v)晶场中d~3离子吸收谱的理论研究

为了计算Cr~(3+)离子在C_(3v)对称晶场中的能谱,本文采用一种形式介于Richardson和Watson SCF波函数之间的束缚态d电子径向轨函;从Oh点群的Griffith标准基出发,用一种简便的方法,推出d~3系的C_(3v)点群强场谱项能量矩阵。由此计算了Ruby(Al_2O_3+Cr~(3+))和Cr_2O_3晶体中Cr~(3+)离子的吸收谱。在考虑扳——电耦合后,理论结果与实验符合甚好,从而解释了这两类晶体中Cr~(2+)吸收光谱的机制。这种计算方法既使拟合参数的数目大为减少,又使配位场理论计算格地理论化。     

d~5系C_(2h)点群强场方案和MnCl_2·2H_2O的吸收谱

利用一种处理低对称络离子吸收谱强场方案,推出d~5系C_(2h)点群不可约表示对应的能量矩阵。考虑振动电子偶合及双电子激发,解释了MnCl_2·2H_2O晶体中Mn~(2+)的复杂吸收谱。确认了Mn~(2+)络离子晶场的C_(2h)对称性。     

假四面体(C2v)钴(Ⅱ)配合物电子光谱的强场处理

钴(Ⅱ)的假四面体(C_(2v))配合物 CoL_2X_2的配体场光谱一般显示出两组谱带,分别对应于基态~4A_2对两个~4T_1谱项的三个低对称性分量~4B_1,~4A_2和~4B_2的跃迁。前人对这类光谱的处理多采用弱场近似,模型多采用点电荷模型,结果得到的跃迁能和实测值相差较大。Menzel等指出:简单点电荷模型的固有弊病使得它不可能对此类共价配合物的光谱作出理想的处理。他们对点电荷模型作了适当的修改,应用弱场近似取得了满意的结果。本文应用强场近似处理这类配合物的光谱,和修改的点电荷模型相比较我们的结果更为满意。     

Co(Ⅱ)、Ni(Ⅱ)与二氮杂18-冠-6配合物的研究——Ⅱ.Ni(NCS)2、Ni(NO3)2与1,7,10,16-四氧杂-4,13-二氮杂环十八烷配合物的合成和Ni(NCS)2与该配体配合物的结构

本文报道Ni(NCS)_2·4H_2O,Ni(NO)·6H_2O与1,7,10,16—四氧杂—4,13—二氮杂环十八烷形成的配合物,测定了配合物的红外光谱、电导、电子光谱、磁性以及差热—热重分析,根据电子光谱对Ni(Ⅱ)离子的d—d跃迁进行了指派,并计算D_q值和B值,测定了Ni(NCS)_2C_(12)H_(26)O_4N_2配合物的晶体和分子结构,晶体属单斜晶系,空间群P2_1/a,a=7.512(1)A,b=8.524(1)A,c=15.286(3)A,β=100.29(1)A,V=963.05A,Z=2。结构通过Patterson法解出,最终偏离因子R=0.027。分子结构中Ni(Ⅱ)离子同大环配体的两个氮原子和两个氧原子以及NCS-中的两个氮原子配位,形成六配位的畸变八面体。     

铍-铍金属链夹心配合物D_(4d)[Be_n(C_4H_4)_2]~(2-)及[Be_n(C_4H_4)_2]Li_2(n=2~8)（英文）

采用密度泛函理论方法(B3LYP和BP86)在6-311+G(d,p)基组水平上系统研究了新颖的铍-铍金属链夹心配合物D_(4d)[Be_n(C_4H_4)_2]~(2-)及[Be_n(C_4H_4)_2]Li_2(n=2~8)的几何结构、电子结构、成键特征及热力学稳定性。结果表明,具有交错式D4d对称性的D_(4d)[Be_n(C_4H_4)_2]~(2-)及[Be_n(C_4H_4)_2]Li_2为体系势能面上的真正极小。自然键轨道(NBO)、分子中的原子(AIM)及分子轨道分析表明,该系列夹心配合物中铍-铍间主要以共价键为主,而配体与铍-铍链之间则主要以离子键为主。核独立化学位移(NICS)分析表明配体在该系列配合物中具有π芳香性。稳定的夹心配合物锂盐[Be_n(C_4H_4)_2]Li_2(n=2~8)有望通过C4H4Li2/C5H-5配体交换反应进行制备,该系列配合物将进一步丰富多核夹心配合物研究领域。     

双齿配体八配位镧系配合物的结构化学研究——La[(S2CNC4H8)3·C4H8O·H2O]的合成和晶体结构

镧的配合物La[(S_2CNC_4H_8)_3·C_4H_8O·H_2O]是由LaCl_3和Na(S_2CNC_4H_8)·2H_2O在四氢呋喃中反应而获得的。它的晶体属于三斜晶系,空间群为Pi,单胞参数a=10.557(2)(?),b=10.943(3)(?),c=13.443(3)(?),α=101.83(2)(?),β=9306(2)°,γ=114.90(2)°,V=1391.9(1.5)(?)~3,Z=2。 晶体结构是采用Patterson法和几轮的差Fourier合成解出的。所有非氢原子的位置参数和各向异性热振动参数经全矩阵最小二乘法修正,最后偏离因子R=0.032,R_w=0.046。分子结构中La原子同三个(S_2CNC_4H_8)~-中的六个S原子和分别来自四氢呋喃分子和水分子中的二个O原子键联。La—S平均距离2.973(?),La—O距离分别为2.596(?)(THF)和2.555(?)(H_2O),它们形成一个扭变三角形十二面体的配位多面体构型。     

硝酸铈(Ⅲ)与二缩三乙二醇-二-(8′-喹啉)醚配合物〔Ce(C24H25N2O4)(NO3)4〕的分子结构

硝酸铈(Ⅲ)与二缩三乙二醇-二-(8’-喹啉)醚(L)的配合物[Ce(C_(24)H_(25)N_2O_4)(NO_3)_4]晶体属三斜晶系,PT空间群;α=9.579(3),b=12.548(2),c=13.801(2)A,α=106.36(1),β=86.12(2),γ=112.43(2)°,V=1469.58A~3;Z=2,D_6=1.99g/cm~3;R=0.019。在配合物的分子中Ce~(3+)与L的一个喹啉N原子三个醚氧原子和四个双齿配位NO_3中的八个氧原子配位,铈的配位数为12。分子中有一个氢离子与另一个喹啉N原子结合并与硝酸根的氧原子形成氢键,从而使配合物分子在能量上得到补偿。     

混合簇合物(G_5H_5FeC_5H_4C_2Ph)Co_2(CO)_6的结构研究

本文用电化学方法和X射线单晶结构分析,研究了混合簇合物(C_5H_5FeC_5H_4C_2Ph)Co_2(CO)_6的结构。由循环伏安结果,分别讨论了簇合物中C_5H_5FeC_5H_4和C_2Co_2中心的成键性质,X射线单晶结构分析表明:晶体属单斜晶系,空间群为P2_1,晶胞参数a=11.845(6),b=8.155(6),c=24.031(6) ,β=90.88°,晶胞中分子数Z=4,密度D_0=1.637g·cm~(-3),分析了(C_5H_5FeC_5H_4C_2Ph)Co_2·(CO)_6的结构特点,并从成键角度讨论了(RC_2R~1)Co_2(CO)_6类簇合物的结构随RC_2R~1不同而变化的规律。     

原子簇配合物〔(C_4H_9)_4N〕_2〔Mo_2S_6O_2〕的合成、结构和性质研究

用(NH_4)_2MoS_4、FeCl_3和(C_4H_9)_4NBr在CH_3OH-CH_3ONa溶液中反应,得到了原子簇配合物[(C_4H_9)_4N]_2[Mo_2S_6O_2]晶体,用X-射线单晶衍射方法测定了簇合物的晶体结构,晶体属空间群D_(2h)~(15)-P_(c a h),晶胞参数为a=15.876(3),6=17.786(6),c=31.90(1),V=9008.7~3,经块矩阵最小二乘法修正,最终得偏离因子R=0.0659,同时对簇合物的红外光谱、拉曼光谱、紫外可见光谱以及电化学性质也进行了研究。     

Raman,infrared and force field studies of K2(12)C2O4 x H2O and K2(13)C2O4 x H2O in the solid state and in aqueous solution,and of (NH4)2(12)C2O4 x H2O and (NH4)2(13)C2O4 x H2O in the solid state

The Raman and infrared spectra of solid K2(12)C2O4 x H2O are reported together with, for the first time, the corresponding Raman and infrared spectra of solid K2(13)C2O4 x H2O. Raman spectra of aqueous solutions of both isotopomers are also reported. In the solid state the oxalate anion is planar with D2h symmetry in this salt, whereas in aqueous solution the Raman spectra of the anion are best interpreted on the basis of D2d symmetry. The Raman spectra of solid (NH4)2(12)C2O4 x H2O and (NH4)2(13)C2O4 x H2O, in which the oxalate anion is twisted from planarity by 28 degrees about the CC bond, have also been recorded. Several reassignments have been made. The harmonic force field for the oxalate anion in the D2h, D2 and D2d geometries has been determined in part, and approximate values of key valence force constants determined. All the observed band wavenumbers and 12C/13C isotopic shifts are well reproduced by the force fields. The potential energy distribution of the totally symmetric normal modes of planar oxalate indicates that each mode consists of extensively mixed symmetry corrdinates and that the labels previously used for the bands seen here at 475 and 879 cm(-1) would better be described as v(CC) and deltaS(CO2), respectively, putting them in the same wavenumber order as v(NN) and deltaS(NO2) for the isoelectronic and isostructural molecule N2O4. The stretching force constants of N2O4 and planar C2O4(2-) are established to be in the order f(NN) < f(CC) and f(NO) > f(CO), consistent with the known relative bond lengths.     

丙二烯分子的模糊对称性

利用作者提出的探讨分子及其轨道模糊对称性的方法分析了丙二烯在内旋转过程中模糊对称性特征. 考虑到此过程中经历不同状态所属的对称点群, 即D2h、D2d与D2. 利用包含这些点群中所有元素的最小点群D4h进行分析. 将D4h中的元素分为四组: (i) G0——包含在D2点群中的元素, 也是所有上述点群中都存在的元素; (ii) G1——包含在D2h点群中, 但不包含在D2d点群中的元素; (iii) G2——包含在D2d点群中, 但不包含在D2h点群中的元素; (iv) G3——包含在D4h点群中, 但不包含在D2h与D2d点群中的元素. 分别分析在内旋转过程中各个分子轨道(MO)相应每一组元素的隶属函数的共性变化规律性.     

PdH2、YH2分子的结构与势能函数

用密度泛函理论的B3LYP方法,对钯和钇原子采用SDD收缩价基函数,氢原子采用6-311＋＋G**全电子基函数,对PdH2和YH2体系的结构进行优化计算,得到PdH2分子最稳态为C2v构型,电子组态为1A1,平衡核间距RPdH=0.1692 nm,键角∠HPdH=29.4°,离解能De=5.5212 eV,基态简正振动频率:ν1(b2)=1470.1 cm－1、ν2(a1)=1007.9 cm－1、ν3(a1)=2907.0 cm－1.YH2分子最稳态也为C2v构型,电子组态2A1,RYH=0.1962 nm,∠HYH=114.3°,De=5.6691 eV,基态简正振动频率:ν1(b2)=1457.9 cm－1、ν2(a1)=476.0 cm－1、ν3(a1)=1506.3 cm－1.由微观过程的可逆性原理分析了分子的可能离解极限.并用多体项展式理论方法分别导出基态PdH2和YH2分子的势能函数,其等值势能面图准确地再现了PdH2和YH2分子的结构特征和离解能,由此讨论了Pd ＋ H2和Y ＋ H2分子反应的势能面静态特征.     

The Fuzzy D2h-symmetries of Ethylene Tetra-halide Molecules and their Molecular Orbitals

Based on our study in relation to the fuzzy symmetry characterization and the application to linear molecule, the fuzzy symmetry of the planar molecules have been analyzed. The prototypical planer molecules we have chosen to study are the C2F3X (X = Cl, Br, and I) and three kinds of C2F2Cl2 isomers. These molecules relate to the fuzzy symmetry in connection with the D2h point group. As we known, the D2h point group includes an identity transformation and seven twofold symmetry transformations but without higher-fold ones. Meanwhile, it is related only to some one-dimensional irreducible representations, but there is not to multi-dimensional irreducible representation. In this paper, the fuzzy symmetries of these molecules and their molecular orbital(MO)s have been studied, such as the membership functions, the representation compositions, the fuzzy correlation diagrams and so on have been analyzed. These analysis methods can be used to analyze the molecular fuzzy symmetries of some other molecule systems, no difficulty.     

Electron spin resonance study on H6+, H5D+, H4D2+, and H2D4+ in solid parahydrogen

We carried out an electron spin resonance (ESR) study on hydrogen ion radicals produced by radiolysis of solid para-H(2). In addition to quartet ESR lines proposed to be H(2) (+)-core H(6) (+) (D(2d)) ions in solid para-H(2) [T. Kumada et al., Phys. Chem. Chem. Phys. 7, 776 (2005)], we newly observed totally more than 50 resolved lines in gamma-ray irradiated solid para-H(2)-ortho-D(2) (1 mol %) and para-H(2)-HD (1 mol %) mixtures. We assigned these lines to be isotope substituents of H(2) (+)-core H(6) (+) ions such as H(5)D(+), H(4)D(2) (+), and H(2)D(4) (+) throughout the comparison of their ESR parameters with theoretical results. These results provide a conclusive evidence that H(2) (+)-core H(6) (+) ions are generated in irradiated solid hydrogens. Analysis of the EPR spectrum and ab initio calculations predicts D(2d) symmetry of the H(6) (+) ions, whereas a lowering symmetry (D(2d)-->C(2v)) induced by asymmetric nuclear wave function is observed in H(5)D(+) and H(4)D(2) (+). We also observed isotope-substitution reactions such as H(6) (+)+D(2)-->H(4)D(2) (+)+H(2) and H(6) (+)+HD-->H(5)D(+)+H(2), which are analogous to the well-known isotope-condensation reactions of H(3) (+) in dark nebula, H(3) (+)+HD-->HD(2) (+)+H(2) and HD(2) (+)+HD-->D(3) (+)+H(2).     

d^3的C2v电子能级和CoCl4^2电子光谱解析

本文计算了d^3电子组态在C2v场中的全部能量矩阵元, 微扰算符包括静电算符、晶场算符和旋轨偶合算符, 讨论了拟合了Cs2CoCl4的电子光谱。     

Infrared spectra of C(3)H(3)(+)-N(2) dimers: identification of proton-bound c-C(3)H(3)(+)-N(2) and H(2)CCCH(+)-N(2) isomers.

Mid-infrared photodissociation spectra of mass selected C(3)H(3)(+)-N(2) ionic complexes are obtained in the vicinity of the C-H stretch fundamentals (2970-3370 cm(-1)). The C(3)H(3)(+)-N(2) dimers are produced in an electron impact cluster ion source by supersonically expanding a gas mixture of allene, N(2), and Ar. Rovibrational analysis of the spectra demonstrates that (at least) two C(3)H(3)(+) isomers are produced in the employed ion source, namely the cyclopropenyl (c-C(3)H(3)(+)) and the propargyl (H(2)CCCH(+)) cations. This observation is the first spectroscopic detection of the important c-C(3)H(3)(+) ion in the gas phase. Both C(3)H(3)(+) cations form intermolecular proton bonds to the N(2) ligand with a linear -C-H...N-N configuration, leading to planar C(3)H(3)(+)-N(2) structures with C(2v) symmetry. The strongest absorption of the H(2)CCCH(+)-N(2) dimer in the spectral range investigated corresponds to the acetylenic C-H stretch fundamental (v(1) = 3139 cm(-1)), which experiences a large red shift upon N(2) complexation (Delta(v1) approximately -180 cm(-1)). For c-C(3)H(3)(+)-N(2), the strongly IR active degenerate antisymmetric stretch vibration (v4)) of c-C(3)H(3)(+) is split into two components upon complexation with N(2): v4)(a(1)) = 3094 cm(-1) and v4)(b(2)) = 3129 cm(-1). These values bracket the yet unknown v4) frequency of free c-C(3)H(3)(+) in the gas phase, which is estimated as 3125 +/- 4 cm(-1) by comparison with theoretical data. Analysis of the nuclear spin statistical weights and A rotational constants of H(2)CCCH(+)-N(2) and c-C(3)H(3)(+)-N(2) provide for the first time high-resolution spectroscopic evidence that H(2)CCCH(+) and c-C(3)H(3)(+) are planar ions with C(2v) and D(3h) symmetry, respectively. Ab initio calculations at the MP2(full)/6-311G(2df,2pd) level confirm the given assignments and predict intermolecular separations of R(e) = 2.1772 and 2.0916 A and binding energies of D(e) = 1227 and 1373 cm(-1) for the H-bound c-C(3)H(3)(+)-N(2) and H(2)CCCH(+)-N(2) dimers, respectively.     

Hydrogen bridging in the compounds X2H (X=Al,Si,P,S)

X2H hydrides (X=Al, Si, P, and S) have been investigated using coupled cluster theory with single, double, and triple excitations, the latter incorporated as a perturbative correction [CCSD(T)]. These were performed utilizing a series of correlation-consistent basis sets augmented with diffuse functions (aug-cc-pVXZ, X=D, T, and Q). Al2H and Si2H are determined to have H-bridged C2v structures in their ground states: the Al2H ground state is of 2B1 symmetry with an Al-H-Al angle of 87.6 degrees, and the Si2H ground state is of 2A1 symmetry with a Si-H-Si angle of 79.8 degrees. However, P2H and S2H have nonbridged, bent Cs structures: the P2H ground state is of 2A' symmetry with a P-P-H angle of 97.0 degrees, and the S2H ground state is of 2A' symmetry with a S-S-H angle of 93.2 degrees. Ground state geometries, vibrational frequencies, and electron affinities have been computed at all levels of theory. Our CCSD(T)/aug-cc-pVQZ adiabatic electron affinity of 2.34 eV for the Si2H radical is in excellent agreement with the photoelectron spectroscopy experiments of Xu et al. [J. Chem. Phys. 108, 7645 (1998)], where the electron affinity was determined to be 2.31+/-0.01 eV.     

On the equilibrium structures of the complexes H2C3H+ · Ar and c-C3H3(+) · Ar: results of explicitly correlated coupled cluster calculations

Explicitly correlated coupled cluster theory at the CCSD(T)-F12x (x = a, b) level [T. B. Adler et al., J. Chem. Phys. 127, 221106 (2007)] has been employed in a study of the potential energy surfaces for the complexes H(2)C(3)H(+) · Ar and c-C(3)H(3)(+) · Ar. For the former complex, a pronounced minimum with C(s) symmetry was found (D(e) ≈ 780 cm(-1)), well below the local "H-bound" minimum with C(2v) symmetry (D(e) ≈ 585 cm(-1)). The absorption at 3238 cm(-1) found in the recent infrared photodissociation spectra [A. M. Ricks et al., J. Chem. Phys. 132, 051101 (2010)] is, thus, interpreted as an essentially free acetylenic CH stretching vibration of the propargyl cation. A global minimum of C(s) symmetry was also obtained for c-C(3)H(3)(+) (D(e) ≈ 580 cm(-1)), but the energy difference with respect to the local C(2v) minimum is only 54 cm(-1).     

Sequestered plutonium: [Pu(IV){5LIO(Me-3,2-HOPO)}2]--the first structurally characterized plutonium hydroxypyridonate complex

The first single-crystal X-ray diffraction analysis of a hydroxypyridonate plutonium(IV) complex is presented, that of the tetradentate ligand 5LIO(Me-3,2-HOPO) with Pu(IV). The [Pu(IV){5LIO(Me-3,2-HOPO)}(2)] complex crystallizes in the space group Pna2(1) with the asymmetric unit cell containing two unique eight-coordinate plutonium complexes and one perchlorate anion. According to shape measure analysis, the geometry of both Pu centers is closest to a bicapped trigonal prism (C(2v) symmetry, for Pu 1: S(C(2v))=13.48 degrees , S(D(4d))=15.43 degrees , S(D(4d))=16.10 degrees ). The average bond length for the Pu--O(phenolic) is 2.31(4) A, whereas the Pu--O(amide) distances are slightly longer, averaging 2.40(2) A. The preparative chemistry of this compound and the implications of the structure are discussed.