HPO_2异构体结构和相对稳定性

在MP2/6-311++G（d,p）和QCISD（t）/6-311++G（3df,2p）（单点）水平下计算得到了包括8个异构体和12个过渡态的HPO2体系势能面.在势能面上,异构体cis-HOPO（EI）的能量是最低的,其次是trans-HOPO（E2）和HPO（O）（C2v,E3）,能量分别比cis-HOPO高10.99和48.36 kJ/mol.根据体系的势能面,只有异构体E1和E3具有较高的动力学稳定性,在实验中应该可以观测到.PH和O2直接反应生成的cis-HPOO（E5）和trans-HPOO（E6）经过几步势垒较低的异构化过程就可以异构化为具有较高动力学稳定性的产物E1;而OH和PO反应可直接生成E1.计算结果较好地解释了相关实验.     

HPOS体系异构体结构与稳定性

在MP2／6－311＋＋G(d,p)和QCISD（T）／6－311＋＋G（3df,2p)（单点）水 平下计算得到了HPOS体系势能面上18个异构体和25个过渡态及解离碎片等驻点，并 分析了这些异构体的结构及异构化过程，讨论了可能的解离方式。在得到的异构体 中，有8个异构体是动力学较稳定的，它们是dis-HOPS,trans-HOPS,trans-HSPO, cis-HSPO,HP(O)S(Cs),trans-HPSO,cis-HPSO和HP（O）S（C1）。这些异构体在实 验中应该可以观测到。理论研究表明，P与S原子较强的超价能力在降低异构体能量 ，提高异构体动力学稳定性方面起到了关键的作用。得到的计算结果与HPO2， HPS2，HNOS等价电子相同的体系进行了比较。     

HAsO~2异构体结构、相对稳定性与体系势能面

在MP2/6-311++G(d,p)和QCISD(T)/6-311++G(3df,2p)(单点)水平下计算得到了包括9个异构体和10个过滤态的HAsO~2体系势能面。在势能面上，异构体cis-HOAsO(E1)的能量是最低的，其次是trans-HOAsO(E2)和HAsO(O)(C~2~V,E3)，能量分别比cis-HOAsO高13.15和192.74kJ/mol。根据体系的势能面，异构体E1，E3及cis-HOOAs(E6),trans-HOOAs(E5)具有一定的动力学稳定性，在实验中应该可以观测到。AsH和O~2反应的第一步产物将会异构化为具有较高动力学稳定性的异构体E3；而OH和AsO反应可直接生成E1。计算结果与HPO~2,HPS~2,HNO~2,HNS~2等价电子相同的分子的势能面进行了比较。     

HPO2异构体结构和相对稳定性

在MP2/6-311++G(d,p)和QCISD(t)/6-311++G(3df,2p)(单点)水平下计算得到了包括8个异构体和12个过渡态的HPO₂体系势能面. 在势能面上, 异构体cis-HOPO(E1)的能量是最低的, 其次是trans-HOPO(E2)和HPO(O)(C_2V, E3), 能量分别比cis-HOPO高10.99和48.36 kJ/mol. 根据体系的势能面, 只有异构体E1和E3具有较高的动力学稳定性, 在实验中应该可以观测到. PH和O₂直接反应生成的cis-HPOO(E5)和trans- HPOO(E6)经过几步势垒较低的异构化过程就可以异构化为具有较高动力学稳定性的产物E1; 而OH和PO反应可直接生成E1. 计算结果较好地解释了相关实验.     

HAsS2异构体结构与稳定性

在MP2/6-311++G(d,p)和QCISD(t)/6-311++G(3df,2p)(单点)水平下计算得到9个异构体和10个过渡态的HAsS₂体系势能面.异构体cis-HSAsS(E1)的能量最低,其次是trans-HSAsS(E2)、具有AsSS三元环的立体HAs(S)S(C_{s,E3)和HAs(S)S(C2v,E4)结构的异构体,能量分别比cis-HSAsS高1.46,60.78和93.63kJ/mol.根据体系的势能面,异构体E1,E2,E3和E4具有一定的动力学稳定性.AsH和S2第一步反应产物将会异构化为具有较高动力学稳定性的异构体E3,而SH和AsS第一步反应产物将会异构化为E1.计算结果与HNO2,HNS2,HPO2,HPS2和HAsO2等价电子相同的分子的势能面进行了比较.}     

HBO2异构体的结构和相对稳定性

用ab initio方法在MP2/6 311＋＋G(d,p)水平下优化得到了HBO2体系的若干异构体和过渡态，并在QCISD(t)/6 311＋＋G(3df,2p)//MP2/6 311＋＋G(d,p)水平下进行了单点能量校正.对计算结果的分析表明，无论是在热力学还是在动力学上，具有链状结构的HOBO异构体(E1)是势能面上最稳定的结构，并对E1的电子结构进行了分析；另一具有C2v对称性的HBO(O)结构的异构体(E2)的能量比E1高381.72 kJ•mol－1，由于E2处于一个较深的势垒中，因此是比较稳定的，可以推断，在适合的实验中应该可以观察到异构体E2.     

NC3O分子体系的异构化及其结构和性能的理论研究

采用 DFT, QCISD 及 CCSD(T)方法, 对 NC3O 分子体系的异构化进行了系统的研究, 得到了5个稳定的异构体, 其中包括4个链状异构体和1个带有支链的平面结构异构体. 这5个稳定异构体都具有较高的动力学和热力学稳定性.     

[Co(3,3-tri)(amp)Cl]~(2+)四个经式异构体取代、重排反应及其与结构关系的研究

对犤Co(3,3-tri)(amp)Cl犦2+四个几何经式异构体在不同条件下的取代及重排反应进行考察的实验结果表明,四个几何经式异构体碱性环境下的水解速率没有显著的差异,cis异构体比trans异构体约快20倍。实验中没有观察到面式异构体。在100℃二甲亚砜中加热的重排反应实验中可观察到异构体进行配体翻转的历程,如异构体m1-Cl转化为m4-Cl,m2-Cl转化为m3-Cl。m3和m4相对较稳定。利用量子化学从头计算法,在赝势基组RHF/LANL2DZ的水平上对该体系各异构体进行了基态能量、几何优化的计算,与已测定的异构体m3犤ZnCl4犦H2O和m4犤ZnCl4犦晶体结构参数比较,键长及键角的相对误差不超过3%。根据各异构体基态能量说明了各异构体的平衡分布;讨论了键角变形性大小与各异构体反应性大小的关系。     

[Si,N,N,P]体系异构体结构与稳定性

在B3LYP/6-311G(d)和QCISD(t)/6-311+G(2df)(单点)水平下计算得到了[Si,N,N,P]体系势能面上的一些驻点, 研究了异构体之间的异构化过程, 并讨论了该体系异构体的结构与稳定性. 结果表明在[Si,N,N,P]体系中的11个异构体中只有含有Si-P交叉成键的类蝶型四元环异构体SiNPN(E1, ²A″)是稳定的, 其他异构体由于易于重排或是解离, 稳定性较低. 研究同时给出了E1的电子与几何结构、振动频率及指认、偶极矩和转动常数等相关数据. 分析结果表明通过中间体E3(SiNPN)的反应SiN(²Π) + PN(¹Σ)→E1是由SiN(²Π)和PN(¹Σ)碎片产生E1的最有利途径, 因此E1可成为星际观测的目标. G2级别下此反应的反应焓变为215.25 kJ/mol (298.15 K), 而异构体E1在298.15 K下的标准生成焓为457.99 kJ/mol.     

磷炔R-C≡P(R=-BH2,-CH3,-NH2,-OH)及其异构体的稳定性

采用 B3LYP和 CCSD(T)方法对 R-C≡ P(R=-BH2, -CH3,-NH2, -OH)体系进行了理论研究 .结果表明,含 C≡ P三键的异构体 BH2-C≡ P和 CH3-C≡ P在各自的体系中分别是热力学最稳定的结构 .而在 HO-C≡ P和 NH2-C≡ P体系中,热力学最稳定的结构却是 H-P=C=O和含 C≡ N三键的 N≡ C-PH2.动力学理论研究表明,没有相关实验研究的 R-C≡ P(R=-BH2,NH2)体系中共有 5种异构体是动力学稳定的 .在 HO-C≡ P体系的 2种动力学稳定的异构体中, H-P=C=O连接方式的异构体已被实验所证实,而另外一种 HO-C≡ P连接方式的异构体的动力学稳定性较高,实验中可以观察到 .对于 CH3C≡ P体系,研究所预示的 2种动力学稳定的异构体中 CH3-C≡ P已被实验证实,从理论上推测另一种动力学稳定性较高的异构体 HC≡ C-PH2在实验中也可以检测到.     

Solid state coordination chemistry: construction of 2D networks and 3D frameworks from phosphomolybdate clusters and binuclear Cu(II) complexes. The syntheses and structures of [(Cu2(tpypyz)(H2O)2)(Mo5O15)(HOPO3)2].nH2O [n = 2, 3; tpypyz = tetra(2-pyridyl)pyrazine

The hydrothermal reaction of MoO3, Cu(C2H3O2)2.H2O, tpypyz, H3PO4 and H2O yields a 2D material, [(Cu2(tpypyz)(H2O)2)(Mo5O15)(HOPO3)2].2H2O (1.2H2O), constructed from (Mo5O15(HOPO3)2)4- clusters linked through (Cu2(tpypyz)(H2O)2)2+ components; in contrast, use of Cu2O in the synthesis in place of Cu(C2H3O2)2.H2O yields a 3D material [(Cu2(tpypyz)(H2O)2)(Mo5O15)(HOPO3)2].3H2O (2.3H2O), constructed from the same building blocks as 1.2H2O.     

Structures and stabilities of HPO_2 isomers

The potential energy surface of HPO2 system including eight isomers and twelve transition states is predicated at MP2/6-311++G(d, p) and QCISD(t)/6-311++G(3df,2p)(single-point) levels of theory. On the potential energy surface, cis-HOPO(E1) is found to be thermodynamically and kinetically most stable isomer followed by trans-HOPO(E2) and HPO(O)(C2v, E3) at 10.99 and 48.36 kJ/mol higher, respectively. Based on the potential energy surface, only E1 and E3 are thermodynamically stable isomers, and should be experimentally observable. The products cis-HPOO(E5) and frans-HPOO(E6) in the first-step reaction of HP with O2 can isomerize into isomer E1 that has higher stability. The reaction of OH with PO will directly lead to the formation of isomer E1. The computed results are well consistent with the previous experimental studies.     

Monitoring dehydration and condensation processes of Na2HPO4*12H2O using thermo-Raman spectroscopy

Thermal dehydration and condensation processes of disodium hydrogen phosphate dodecahydrate (Na2HPO4*12H2O) were monitored by thermo-Raman spectroscopy (TRS). Various hydrated forms Na2HPO4*12H2O, Na2HPO4*8H2O, Na2HPO4*7H2O, Na2HPO4*2H2O, Na2HPO4*H2O and Na2HPO4 were observed, followed by condensation of Na2HPO4 to sodium pyrophosphate (Na4P2O7) in a dynamic thermal process. Representative Raman spectra of all the hydrated forms Na2HPO4*12H2O, Na2HPO4*8H2O, Na2HPO4*7H2O, Na2HPO4*2H2O, Na2HPO4*H2O and Na2HPO4 were detected in both H2O and PO4(3- )regions are reported. The thermo-Raman intensity (TRI) thermogram also showed systematic loss of water in five steps of dehydration, with the differential TRI thermogram in agreement shows five dips corresponding to the five steps of dehydration, respectively. Thermogravimetry (TG) and differential thermogravimetry (DTG) are in harmony with the results of TRS, though, the two could not resolve the steps involved.     

An approach to the synthesis of polyoxometalate encapsulating different kinds of oxoanions as heteroions: bisphosphitopyrophosphatotriacontamolybdate [(HPO3)2(P2O7)Mo30O90]8-

A yellow [(HPO(3))(2)(P(2)O(7))Mo(30)O(90)](8-) anion was prepared as a tetrapropylammonium (Pr(4)N(+)) salt from a 50 mM Mo(VI)-2 mM P(2)O(7)(4-)-4 mM HPO(3)(2-)-0.95 M HCl-60% (v/v) CH(3)CN system at ambient temperature. The (Pr(4)N)(8)[(HPO(3))(2)(P(2)O(7))Mo(30)O(90)] salt crystallized in the orthorhombic space group P(nma) (No. 62), with a = 30.827(2) A, b = 22.8060(15) A, c = 30.928(2) A, V = 21743(3) A(3), and Z = 4. The structure contained a (P(2)O(7))Mo(12)O(42) fragment derived from the removal of each corner-shared Mo(3)O(13) unit in a polar position from a [(P(2)O(7))Mo(18)O(54)](4-) structure, and each side of the (P(2)O(7))Mo(12)O(42) fragment was capped by a B-type (HPO(3))Mo(9)O(24) unit. The [(HPO(3))(2)(P(2)O(7))Mo(30)O(90)](8-) anion was characterized by voltammetry and IR, UV-vis, and (31)P NMR spectroscopy. Unlike the Keggin and Dawson anions and the parent [(P(2)O(7))Mo(18)O(54)](4-) anion, the [(HPO(3))(2)(P(2)O(7))Mo(30)O(90)](8-) anion exhibited two-electron redox waves in CH(3)CN with and without acid.     

Syntheses, structures, and magnetic properties of inorganic-organic hybrid cobalt(II) phosphites containing bifunctional ligands

Seven new cobalt(II) phosphites, [Co(HPO(3))(C(14)H(14)N(4))(H(2)O)(2)].2H(2)O (1), [Co(HPO(3))(C(22)H(18)N(4))].H(2)O (2), [Co(2)(HPO(3))(2)(C(22)H(18)N(4))(2)H(2)O].H(2)O (3), [Co(2)(HPO(3))(2)(C(12)H(10)N(4))(1.5)H(2)O].1.5H(2)O (4), [Co(HPO(3))(C(14)H(14)N(4))(0.5)].H(2)O (5), [Co(HPO(3))(C(18)H(16)N(4))(0.5)] (6), and [Co(HPO(3))(C(18)H(16)N(4))(0.5)] (7) were synthesized in the presence of 1,2-bis(imidazol-1-ylmethyl)benzene (L1), 1,4-bis(benzimidazol-1-ylmethyl)benzene (L2), 1,3-bis(benzimidazol-1-ylmethyl)benzene (L3), 1,4-bis(1-imidazolyl)benzene (L4), 1,4-bis(imidazol-1-ylmethyl)benzene (L5), 1,4-bis(imidazol-1-ylmethyl)naphthalene (L6), and 1,5-bis(imidazol-1-ylmethyl)naphthalene (L7), respectively, and their structures were determined by X-ray crystallography. Compound 1 is a molecular compound in which two cobalt(II) ions are held together by double mu-O linkages. The inorganic framework of compounds 2 and 3 are composed of vertex-shared CoO(2)N(2)/CoO(3)N(2) and HPO(3) polyhedra that form four rings; these are further linked by an organic ligand to generate 2D sheets. Compounds 4 and 5 both have 1D inorganic structures, with the bifunctional ligands connected to each side of the ladder by coordination bonds to give 2D hybrid sheets. A 3D organically pillared hybrid framework is observed in 6 and 7. In 6, the stacking of the interlayer pillars gives rise to a small hydrophobic channel that extends through the entire structure parallel to the sheets. The temperature-dependent magnetic susceptibility measurements of these compounds show weak interactions between the metal centers, mediated through the mu-O and/or O-P-O linkages.     

稀土亚磷酸盐GdxTb2-x（HPO3）3（H2O）2（0≤x≤2）的微波合成、表征与性质研究

利用微波辅助合成法,成功地合成出一系列新颖的稀土亚磷酸盐GdxTb2-x(HPO3)3(H2O)2(0≤x≤2).X-射线粉末衍射分析结果表明,它们为同构的化合物.对Gd2(HPO3)3(H2O)2进行X-射线单晶衍射分析得出,该化合物结晶于P21/c空间群,晶胞参数为a=6.9124(6),b=12.8891(12),c=12.3692(11),β=100.1520(10)°.Gd2(HPO3)3(H2O)2是由GdO7多面体,GdO8多面体和[HPO3]假四面体通过共用氧原子相互连接而成的三维骨架.Gd2(HPO3)3(H2O)2和Tb2(HPO3)3(H2O)2的荧光光谱分别显示Gd3+和Tb3+的特征发光.Gd/Tb掺杂的样品中存在Gd3+-Tb3+的能量传递,它们的发光显示Tb3+的绿光发射(5D4→7F3-6),并且5D4→7F3跃迁的强度随着Tb3+掺杂量的增大而增强,这表明Gd2(HPO3)3(H2O)2引入不同浓度的发光中心Tb3+之后可以作为绿光发光材料.磁性研究表明,Gd2(HPO3)3(H2O)2中存在极弱的反铁磁相互作用.     

二维层状磷酸亚磷酸钒(Ⅳ)化合物[V2O2(OH)(HPO3)(HPO3)0.7(PO3OH)0.3].(C6N2H16)0.5的水热合成与结构表征

迄今, 在中温水热条件下已合成了大量具有空旷骨架结构的过渡金属磷酸盐微孔材料[1], 这类材料在非线性光学材料、磁性材料、超导材料及催化等诸多方面具有潜在的应用前景[2～5].     

Raman spectroscopy of newberyite, hannayite and struvite

The phosphate minerals hannayite, newberyite and struvite have been studied by Raman spectroscopy using a thermal stage. Hannayite and newberyite are characterised by an intense band at around 980cm(-1) assigned to the v(1) symmetric stretching vibration of the HPO(4) units. In contrast the symmetric stretching mode is observed at 942cm(-1) for struvite. The Raman spectra are characterised by multiple v(3) anti-symmetric stretching bands and v(2) and v(4) bending modes indicating strong distortion of the HPO(4) and PO(4) units. Hannayite and newberyite are defined by bands at 3382 and 3350cm(-1) attributed to HOPO(3) vibrations and hannayite and struvite by bands at 2990, 2973 and 2874 assigned to NH(4)(+) bands. Raman spectroscopy has proven most useful for the analysis of these 'cave' minerals where complex paragenetic relationships exist between the minerals.     

13C NMR, infrared, solvation and theoretical investigation of the conformational isomerism in 1-haloacetones (X = Cl, Br and I)

The solvent dependence of the 13C NMR spectra of chloroacetone (CA), bromoacetone (BA) and iodoacetone (IA) are reported and the 3J(CH) couplings analysed using ab initio calculations and solvation theory. In CA the energy difference (E(cis) - E(gauche)) between the cis (Cl-C-C=O 0 degrees) and gauche (Cl-C-C=O 155 degrees) conformers is 1.7 kcal mol(-1) in the vapour, decreasing to 0.8 kcal mol(-1) in CCl4 solution and to -1.0 kcal mol(-1) in the pure liquid. The conformational equilibrium, in BA, is between the more polar cis (Br-C-C=O 0 degrees) and gauche (Br-C-C=O 132 degrees) conformations. The energy difference (E(cis) - E(gauche)) is 1.8 kcal mol(-1) in the vapour, decreasing to 0.9 kcal mol(-1) in CCl4 solution and to -0.4 kcal mol(-1) in the pure liquid. The energy difference (E(cis) - E(gauche)), in IA, between the cis (I-C-C=O 0 degrees) and gauche (I-C-C=O 104 degrees) conformers is 1.1 kcal mol(-1) in the vapour phase, decreasing to 0.5 kcal mol(-1) in CCl4 solution and to -0.5 kcal mol(-1) in the pure liquid. The vapour state energy difference for BA [1.4 kcal mol(-1) at B3LYP/6-311++G(d,p)] and for IA [1.6 kcal mol(-1) at B3LYP/6-311++G(d,p)/LANL2DZ)] are in very good agreement with the above values. For CA the agreement is also satisfactory [1.4 kcal mol(-1) at B3LYP/6-311++G(d,p)].