B12Sc4和B12Ti4团簇的储氢性质

提出了两个稳定的团簇B₁₂Sc₄和B₁₂Ti₄, 基于理论计算, 研究了它们的结构与储氢性质. 结果发现, 在这两个稳定的团簇中, 过渡金属原子不会聚合在一起而影响它们对氢气的吸附. B₁₂Sc₄最多可以吸附12个氢分子, 达到7.25% (质量分数)的储氢量. 它的平均每氢分子吸附能量为10.5 kJ·mol^-1. B₁₂Ti₄最多只能吸附8个氢分子, 储氢量为4.78%. 但平均每氢分子吸附能量可达50.2 kJ·mol^-1. 进一步计算表明, 即使在77 K,也需要很高的氢气压力才能使12个氢分子都吸附到B₁₂Sc₄上. 电子结构分析表明, B₁₂Ti₄-nH₂吸附结构中的Kubas作用要大于相应B₁₂Sc₄-nH₂结构中的Kubas作用.     

二维TiC 层表面H2的化学吸附与物理吸附

第一性原理计算研究发现由于二维TiC 单原子层具有高的比表面积与大量的暴露在表面的Ti 原子,其是一种非常有潜力的储氢材料. 计算结果显示H₂可以在二维TiC 单原子层表面进行物理吸附与化学吸附. 其中化学吸附能为每个氢分子0.36 eV,物理吸附能是每个氢分子0.09 eV. 覆盖度为1和1/4层（ML）时,H₂分子在二维TiC 单原子层表面的离解势垒分别为1.12 和0.33 eV. 因此,除了物理吸附与化学吸附,TiC 表面还存在H单原子吸附. 最大的H₂储存率可以达到7.69%（质量分数）. 其中,离解的H原子、化学吸附的H₂、物理吸附的H₂的储存率分别为1.54%、3.07%、3.07%. 符合Kubas吸附特征的储存率为3.07%. 化学吸附能随覆盖度的变化非常小,这有利于H₂分子的吸附与释放.     

以还原型钼磷酸盐[P4MoV6O28(OH)3]9-为建筑单元构筑新型多维延展结构材料

向MoO₃, H₃PO₄和bpy(4,4′-bipyridine)组成的反应体系中分别引入Cd(OAc)₂·2H₂O 和MnCl₂·4H₂O, 在水热条件下合成了两种基于还原型钼磷酸盐[P₄Mo₆O₂₈(OH)₃]^9-(简称{P₄Mo₆})为建筑单元构筑的新型多维延展型无机-有机杂化材料(H₂bpy)₂[Cd(H₂O)]₃[Cd(HPO₄)₆(PO₄)₂(OH)₆(MoO₂)₁₂]·5H₂O(1)和 (H₂bpy)₃[Mn(H₂O)₂]₂ [Mn(HPO₄)₆(PO₄)₂(OH)₆(MoO₂)₁₂]·10H₂O(2), 并通过元素分析、红外光谱、热重分析和X射线单晶衍射对其进行了表征。结果表明, 化合物1和2均属于三斜晶系, P1 空间群。化合物1的阴离子[Cd(H₂O)]₃[Cd(HPO₄)₆(PO₄)₂(OH)₆(MoO₂)₁₂]^2-是由二聚体 Cd[P₄Mo₆]₂通过{Cd₃}簇依次连接形成的一维无机链状结构; 化合物2的阴离子[Mn(H₂O)₂]₂[Mn(HPO₄)₆(PO₄)₂(OH)₆(MoO₂)₁₂]^3-则是由二聚体Mn[P₄Mo₆]₂通过Mn²⁺离子连接形成的二维无机层状结构。这2种无机延展结构均同质子化的bpy通过氢键作用形成不同的三维超分子网络。同时还探讨了化合物2的电化学性质。     

N，N′-(2-苯并咪唑基甲基)亚氨基甲基膦酸的双核镍化合物Ni2(bbimp)2(4，4′-bipy)(H2O)2·2H2O和Ni2(bbimp)2(H2O)2][Ni(bbimp)(H2O)2]2·4H2O

该文报道了N，N′-(2-苯并咪唑基甲基)亚氨基甲基膦酸{bbimpH₂，[(C₇H₅N₂)CH₂]₂NCH₂PO₃H₂}的2个镍化合物Ni₂(bbimp)₂(4，4′-bipy)(H₂O)₂·2H₂O (1)和[Ni₂(bbimp)₂(H₂O)₂][Ni(bbimp)(H₂O)₂]₂·4H₂O (2)。化合物1是4，4′-联吡啶作为桥连配体的中性双核结构。化合物2含有1个中性的[Ni₂(bbimp)₂(H₂O)₂]双核分子与2个中性的[Ni(bbimp)(H₂O)₂]单核分子。双核分子单元中的2个Ni(Ⅱ)离子被2个膦酸氧桥连。在化合物2中，膦酸氧桥连的2个Ni(Ⅱ)离子之间存在铁磁性相互作用。     

基于2-硫代巴比妥酸构筑零维原子簇{[Cu6(H2tba)6]·2DMF·xSolvent}、二维层状{[Sc(H2tba)3(DMF)]·2DMF}n和三维网状{[Fe(H2tba)2(H2O)2]·2DMF}n

分别以Cu (ClO₄)₂·6H₂O、Sc (ClO₄)₃·6H₂O和Fe (ClO₄)₃·9H₂O为金属盐,2-硫代巴比妥酸(H₃tba)为配体,通过扩散反应得到了3种不同结构的配合物{[Cu₆(H₂tba)₆]·2DMF·xSolvent}(1)、{[Sc (H₂tba)₃(DMF)]·2DMF}_n(2)和[Fe (H₂tba)₂(H₂O)₂]_n(3),并用红外光谱、元素分析、热重分析和粉末X射线衍射对配合物进行了表征。单晶X射线衍射结构分析表明配合物1是一个具有三方反棱柱构型的六核铜原子簇合物,配合物2是一个具有二维层状结构的化合物,配合物3是一个具有三维网状结构的配位聚合物。配合物1在390 nm光照激发下在735 nm处有强的荧光发射峰。     

半夹芯16电子碳硼烷化合物Me4CpCoS2C2B10H10与二茂铁炔酮的反应性

邻位碳硼烷分别与正丁基锂、硫粉和Me₄CpCo(CO)I₂反应合成得到半夹芯16电子碳硼烷化合物Me₄CpCoS₂C₂B₁₀H₁₀ (1)。1与二茂铁炔酮在二氯甲烷中反应得到产物{(Me₄CpCoS₂C₂B₁₀H₁₀)[FcC(O)CHCCHCC(O)Fc]} (2)(Fc=二茂铁基)。2是一个1:2的加成产物,2个二茂铁炔酮分子以头-尾的方式加成到分子1中的1个Co-S键上。1和2分别用红外、核磁、元素分析、质谱和单晶X-射线衍射等表征方法进行了结构表征。     

“开放型蝶形”[2Fe2S]化合物光催化产氢性能与机理探究

合成并表征了两个新的具有 “开放型蝶形” 结构的[2Fe2S]化合物A和B; 并以A和B为催化剂、 藻红B钠盐 (EBS^2-) 为光敏剂、 三乙胺 (TEA) 为电子给体和质子源, 构建了一个均相光催化产氢体系. 结果表明: 体系在pH为12, 体积比为1∶1的CH₃CN/H₂O溶液中,产氢活性最高,经4 h可见光照射,最大产氢量分别为156.1 μmol (37.9 TON vs. A) 和18.4 μmol (TON 4.6 vs. B); 催化剂中含有质子捕获位点, 有利于形成产氢活性中间体H₂-Fe₂S₂(η²-H²-Fe^IIFe^I) 物种, 从而提高催化剂的产氢活性. 在当前的体系中, 还原态的 Fe^IFe⁰ 物种通过^1* EBS^2-转移到Fe^IFe^I中心上, 然后再经历一个EECC (化合物A) 或ECEC (化合物B), 形成产氢活性中间体H₂-Fe₂S₂(η²-H₂-Fe^IIFe^I)物种, 最终产生H₂分子, 并使Fe^IFe^I 物种再生.     

含膦配体二铁二硫五羰基配合物的合成、表征及电催化产氢性能

本文报道了4个含膦配体二铁二硫五羰基配合物的合成和结构表征。起始配合物[Fe₂(CO)₆(μ-SCH₂CH (CH₂OOCH) S)](1)与三苯基膦、三环己基膦、三(2-甲氧基苯基)膦或三(4-三氟甲基苯基)膦和脱羰试剂Me₃NO·2H₂O反应,以59%~88%的产率制备了目标产物[Fe₂(CO)₅(L)(μ-SCH₂CH (CH₂OOCH) S)](L=PPh₃(2)、PCy₃(3)、P (2-C₆H₄OCH₃)₃(4)、P (4-C₆H₄CF₃)₃(5))。配合物2~5以元素分析、红外光谱、核磁共振以及单晶X射线衍射进行了表征。电化学性质研究表明配合物1~5均可以实现电化学催化质子还原产生氢气的功能,其中配合物1的催化产氢效率明显优于其它配合物。     

Li修饰B12N12储氢行为的密度泛函理论研究

采用基于密度泛函理论(DFT)的第一性原理投影缀加波方法, 研究了Li 修饰的B₁₂N₁₂笼子的储氢行为.计算结果表明: Li 原子吸附在B₁₂N₁₂笼子的四元环和六元环相交的B－N桥位上, 相对于其它六个高对称吸附位置更稳定, B₁₂N₁₂笼子周围最多可以吸附3 个Li 原子, 最稳定的构型是三个Li 原子同时吸附在N原子顶位(Top-N site). 每个Li 原子的周围能吸附三个氢分子, 笼子外侧还可以吸附两个氢分子, 内部最多可以吸附5 个氢分子. 考虑到笼内和笼外的吸附, B₁₂N₁₂笼子总的储氢量(氢分子)达到9.1% (w).     

钴(Ⅲ)催化CpCoS2C2B10H10分子内B(3)/B(6)位和Cp配体偶联

半夹芯16e化合物CpCoS₂C₂B₁₀H₁₀(Cp:cyclopentadienyl) (1)与HC≡CCO₂Me在2-甲基二硫代丙酸存在下反应生成化合物{(C₅H₄CoS₂C₂B₉H₉)(CH=CHCO₂Me)(Me₂C=CS₂H)} (2)和(Me₂C=CS₂H)₃Co (3)。在化合物2中, 原料化合物1中的一个S-Co键断裂, 该S原子与一分子HC≡CCO₂Me末端炔基碳原子连接。Co原子与2-甲基二硫代丙酸的S原子连接成键, 2-甲基二硫代丙酸分子中的SH基团与Co原子通过配位键相连;同时, Cp环的一个碳原子与碳硼烷笼体的B(3)/B(6)位相连, 该B(3)/B(6)位的氢原子迁移到炔烃HC≡CCO₂Me的内部炔基碳原子上形成反式烯键。3个2-甲基二硫代丙酸分子中的3个S原子分别与1中的Co原子通过共价键连接, 3个SH基团与Co原子通过配位键相连, 从而形成化合物3。化合物2和3分别用红外、核磁、元素分析、质谱和单晶X-射线衍射分析等方法进行了表征。     

Synthesis and X-ray diffraction study of R[UO2(CH3COO)3] (R = H3O+ or NH(C2H5) 3+ )

Single crystals of (H₃O)[UO₂(CH₃COO)₃] (I) and (NH(C₂H₅)₃)[UO₂(CH₃COO)₃] (II) are synthesized, and their structures are studied by X-ray crystallography. Compound I crystallizes in the tetragonal crystal system with the unit cell parameters a = 13.70640(10) ?, c = 27.5258(5) ?, V = 5171.14(11) ?³, space group I4₁/a, Z = 16, R = 0.0238. The crystals of compound II are orthorhombic with the parameters a = 13.3685(3) ?, b = 10.6990(3) ?, c = 12.2616(3) ?, V = 1753.77(8) ?³, space group Pna2₁, Z = 4, R = 0.0228. The uranium-containing structural units of crystals I and II are [UO₂(CH₃COO)₃]⁻ island mononuclear groups belonging to the A B₃⁰¹(A = UO₂²⁺, B⁰¹ = CH₃COO⁻) crystal-chemical group of uranyl complexes. [UO₂(CH₃COO)₃]⁻ complexes are linked into a three-dimensional framework by electrostatic interactions with the outer-sphere cations and by hydrogen bonds involving the hydrogen atoms of hydroxonium (I) or triethylammonium (II) with the oxygen atoms of the acetato groups.     

Crystal structures of the novel hydrated borates Ba2B5O9(OH), Sr2B5O9(OH) and Li2Sr8B22O41(OH)2

Three novel hydrated borates Ba₂B₅O₉(OH) (1), Sr₂B₅O₉(OH) (2) and Li₂Sr₈B₂₂O₄₁(OH)₂ (3) have been synthesized hydrothermally and their structures determined. Compounds (1) and (2) are isostructural, crystallizing in space group P2₁/c and having lattice parameters of a=6.6330(13) Å, b=8.6250(17) Å, c=14.680(3) Å, β=93.46(3)° and a=6.4970(13) Å, b=8.4180(17) Å, c=14.177(3) Å, β=94.35(3)°, respectively. Compound (3) crystallizes in P-1 with lattice parameters of a=6.4684(13) Å, b=8.4513(17) Å, c=14.881(3) Å, α=101.21(3)°, β=93.96(3)°, γ=90.67(3)°. While similar in their axis lengths, (3) differs greatly in structure and formulation from (1) and (2). The structure of (1) and (2) is contrasted to that of the well-known mineral hilgardite (Ca₂B₅O₉Cl·H₂O).     

Functionalized boranes for hydrogen storage

Using density functional theory, the generalized gradient approximation for the exchange‐correlation potential and Møller–Plesset perturbation theory we study the hydrogen uptake of Li‐ and Mg‐doped boranes. Specifically, we calculate the structures and binding energies of hydrogen molecules sequentially attached to LiB₆H₇, LiB₁₂H₁₃, Li₂B₆H₆, Li₂B₁₂H_12, MgB₆H₆, and MgB₁₂H₁₂. Up to three H₂ molecules can be bound quasi‐molecularly to each of the metal cations with binding energies per H₂ molecule ranging between 0.07 eV and 0.27 eV. The corresponding gravimetric densities lie in the range of 3.49 to 12 wt %, not counting the H atoms bound chemically to the B atoms.     

Hydrothermal synthesis, characterization and thermochemistry of Ca2[B2O4(OH)2]·0.5H2O

A pure calcium borate Ca₂[B₂O₄(OH)₂]·0.5H₂O has been synthesized under hydrothermal condition and characterized by XRD, FT-IR and TG as well as by chemical analysis. The molar enthalpy of solution of Ca₂[B₂O₄(OH)₂]·0.5H₂O in HC1·54.582H₂O was determined. From a combination of this result with measured enthalpies of solution of H₃BO₃ in HC1·54.561H₂O and of CaO in (HCl + H₃BO₃) solution, together with the standard molar enthalpies of formation of CaO(s), H₃BO₃(s) and H₂O(l), the standard molar enthalpy of formation of −(3172.5 ± 2.5) kJ mol⁻¹ of Ca₂[B₂O₄(OH)₂]·0.5H₂O was obtained.     

Supramolecular Systems Based on Ca2+, [Mo3O2S2Cl6(H2O)3]2s-, [Mo3S4Cl6.75Br0.25(H2O)2]3s- and Cucurbit[6]uril

Adducts of cucurbit[6]uril with Ca²⁺ and trinuclear cluster chloroaquacomplexes (H₉O₄)₂(H₇O₃)₂[(Ca(H₂O)₅)2(C₃₆H₃₆N₂₄O₁₂)]Cl₈·0.67H₂O (1) and [(Ca(H₂O)₅)₂(C₃₆H₃₆N₂₄O₁₂)]× [Mo₃O₂S₂Cl₆(H₂O)₃]₂·13H₂O (2) are obtained and structurally characterized. The structures of both compounds contain polymeric [Ca(H₂O) _n ]₂² CB[6]∞ cations that form infinite columns; the space between them is filled with Cl^s- (1) and [Mo₃O₂S₂Cl₆(H₂O)₃]^2s- (2). A new (H₇O₃)₂(H₅O₂)× [Mo₃S₄Cl_6.25Br_0.25(H₂O)₂](C₃₆H₃₆N₂₄O₁₂)·CH₂Cl₂·6H₂O complex (3) is also obtained and structurally characterized.     

A thermochemical study of dissociative ionization of 4,4-dimethyl-1-thia-4-silacyclohexane and 2,3,3-trimethyl-1-thia-3-silacyclopentane. Decomposition pathways to produce a dimethylsilanethione ion-radical [Me2SiS]+•

The dissociative ionization of 4,4-dimethyl-1-thia-4-silacyclohexane (I) and 2,3,3-trimethyl-1-thia-3-silacyclopentane(II) has been studied by electron photoionization (PI) mass spectrometric methods. The molecular ion fragmentation is mainly related to the loss of ethylene and results in a [Me₂SiSC₂H₄]^+? (m/z 118) ion-radical (A). Further loss of ethylene from A produces a dimethylsilanethione [Me₂SiS]^+? (m/z 90) ion-radical (B). The latter is the most abundant ion in the mass spectra of I and II at 70 eV.The ionization energies (IE) of I (8.22 ± 0.07 eV) and II (8.06 ± 0.03 eV) and the appearance energies (AE) of ion-radicals A and B have been determined. Also, the following heats of formation were calculated (kJ/mol): ΔH_f⁰(I) = ?31.1; ΔH_f⁰(II) = ?65.8; ΔH_f⁰(M_I^+?) = 762.0; ΔH_f⁰(M_II^+?)= 712.1; ΔH_f⁰(A)_aver = 780.2; ΔH_f⁰(B)_aver = 847.7.     

四角锥形结构化合物BeB4X4(X=H，F，Cl)，HBB4H4与BB4H4+中B4平面环的半芳香性

选用6-311++G(3df,2p)基组,在二级微扰的理论下,对四角锥形结构化合物BeB4X4(X=H,F,Cl),HBB4H4与BB4H4+的分子振动频率,及原子间的相互作用进行了计算,作用能的计算使用了CCSD(T)方法。结果显示HBB4H4与BB4H4+是违反韦德规则的另两个特例,它们表现稳定的原因与芳香性有关。     

The H2 elimination reactions of Ã2B3g C2H4+ and C2D4+

Kinetic energy releases from the unimolecular H₂ (D₂) elimination reactions of energy-selected òB_3gC₂H₄⁺(C₂D₄⁺) have been obtained by a photoelectron-photoion coincidence technique. The energy releases suggest a 1,1 elimination and are compatible with the presence of a small reverse activation energy barrier of the order of 0.02 eV. Such a barrier was indicated by a detailed ab initio study of this dissociation and the present results are discussed in the light of this theoretical treatment.     

Tetrahedral complexes of zinc(II) chloride with N- and O-containing organic ligands: Synthesis and crystal structures of [ZnCl2(C12H12N2O)] and [ZnCl2(H2O)2](Me4Pyz)2

New complex chlorides [ZnCl₂(ODA)] (I) (ODA=oxydianiline, C₁₂H₁₂N₂O) and [ZnCl₂(H₂O)₂](Me₄Pyz)₂ (II) (Me₄Pyz = 2,3,5,6-tetramethylpyrazine) were synthesized and crystallographically characterized. Crystals of I are monoclinic, space group C2/c, a = 22.682(2) ?, b = 12.646(1) ?, c = 9.951(1) ?, β = 93.23(2)°, V = 2849.7(5) ?³, ρ_calc = 1.569 g/cm³, Z = 8. Structure I contains cyclic fragments consisting of two tetrahedral complexes (ZnCl₂N₂) and two coordinated bridging oxydianiline ligands. Crystals of II are monoclinic, space group P2(1)/c, a = 8.972(2) ?, b = 13.862(3) ?, c = 17.528(4) ?, β = 101.72(3)°, V = 2134.5(7) ?³, ρ_calc = 1.384 g/cm³, Z = 4. In structure II, supramolecular pseudo-metallocycles are formed due to formation of hydrogen bonds O(w)-H…N between coordinated water molecules and noncoordinated nitrogen atoms of tetramethylpyrazine molecules.