一价阳离子对卟啉二酸H2+4TSPP4-J-聚集的影响

四-(对-磺酸基)苯基卟啉(TSPP4-)作为超灵敏显色剂和电极修饰材料在光谱分析和电化学分析中有重要应用.它在酸性条件下以质子化二酸H24+TSPP4-的形式存在.七十年代,Pasternack等人曾发现H2+4TSPP4-的电子吸收谱随溶液Ph的改变产生复杂的变化,并推测与H2+4TSPP4-的分子缔合有关[1].近年来,H2+4TSPP4-的分子缔合及其光谱性质重新引起人们的兴趣.基于光谱实验结果[2-6],一些作者认为TSPP在强酸性条件下形成准一维的有序结构,类似于菁染料的J-聚集体(Jelley-Scheibe聚集体)[3-5].目前对H2+4TSPP4-J聚集体形成的原因尚不清楚.本文用UV-Vis吸收光谱考察了H+,Li+,Na+,K+对H2+4TSPP4-J聚集的影响,结果显示上述离子的加入可促进H2+4TSPP4-的J-聚集,其中H+起到的促进作用较强.本文还从静电作用的角度,讨论了聚集体中H2+4TSPP4-分子可能的排列方式,并用分子激子理论分析了聚集体激于带的能量,结果与实验基本符合.     

四-(对-磺基苯基)卟啉二酸(H2+4TSPP)分子聚集体的共振喇曼光谱研究

研究了四-(对-磺基苯基)卟啉二酸(H2+4TSPP)的J-聚集体共振喇曼光谱,用氘代法考察了各喇曼谱带的同位素位移.指认3条低波数喇曼带为分子聚集体的晶格模.喇曼光谱退偏比测量表明,聚集体中H2+4TSPP的对称性较分子态降低.比较游离碱H2TSPP和分子态H2+4TSPP共振喇曼光谱讨论了聚集体中H2+4TSPP的结构变化.H2+4TSPP在聚集体中以接近面对面方式排列.     

阴离子开放骨架磷酸盐[Al_4P_5O_(19)(OH)][C_6H_(18)N_2]和[Ga_8P_8O_(32)F_(5.5)][C_6H_(18)N_2]_2[H_3O~+]_(1.5)水热合成中的对映体拆分

以外消旋的2-甲基-1,5-戊二胺(MPMD)为结构导向剂,在水热条件下合成出新磷酸铝化合物[Al4P5O19(OH)][C6H18N2](AlPO-MPMD)和新磷酸镓化合物[Ga8P8O32F5.5][C6H18N2]2[H30+]1.5(GaPO-MPMD).采用单晶x射线衍射结构分析、粉末x射线衍射分析(XRD)、热重-差热分析(TGA-DTA.A)、固体核磁共振(MAs NMR)、旋光分析(Optical rotation)以及振动圆二色光谱分析(Vibrational circular dichroism,VCD)等技术对产物进行了表征.对产物的VCD实验光谱和理论模拟光谱对比分析及旋光分析表明,在水热合成过程中,具有S构象的手性结构导向剂分子比具有R构象的手性结构导向剂分子更多地进入无机化合物骨架中,显示了手性对映体分子在该水热条件下的原位手性拆分.     

一种饱和Keggin硅钨酸盐过渡金属衍生物[Cu(biim)_2]_4[α-SiW_(12)O_(40)]_2·4H_2O（英文）

在水热环境下,将Na10[α-SiW9O34]爛18H2O和CuCl2爛2H2O在2,2′-联咪唑和4,4′-联吡啶存在下反应合成一种饱和Keggin硅钨酸盐杂化物[Cu(biim)2]4[α-SiW12O40]2爛4H2O(1),并通过红外光谱,X射线光电子能谱和X射线单晶衍射进行了结构表征.化合物1分子包含2个中性的Keggin[Cu(biim)2]2[α-SiW12O40]单元和4个结晶水分子.值得注意的是在[α-SiW12O40]4-单元中,与硅原子相连的每个氧原子无序排列在两个位置,这导致了硅原子呈现立方体的几何构型.中性Keggin型[Cu(biim)2]2[α-SiW12O40]单元具有中心对称性,两个[Cu(biim)2]2+配离子对称连接在[α-SiW12O40]4-的两端.邻近的[Cu(biim)2]2[α-SiW12O40]单元之间通过氢键作用形成三维的超分子结构.     

链状三核钼(钨)硫原子簇化合物[M3O2S8]^2^-的合成, 光谱和晶体结构

本文以[NH4]2MOnS4-n(M=Mo, w, n=0-2)为原料, 在酸性和中性条件下, 合成出九个新的三核不对称钼硫和钨硫原子簇状化合物L2[M3O2S8][L=(n-Bu)4N, Ph4P,PyC16H33, (CH3)3NC16H33, Et4N], 用元素分析, 红外光谱, 紫外光谱对簇合物进行了表征, 并测定了其中[(n-Bu)4N]2[Mo3O2S8]和[n-Bu)4N]2[W3O2S8]两个簇合物的晶体结构。本文又一次验证了钼(钨)硫成簇反应是分子内部电子转反应, 并提出了反应历程。     

铍-铍金属链夹心配合物D4d [Ben(C4H4)2]2- 及[Ben(C4H4)2]Li2 (n=2–8)

中文：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[Ben(C4H4)2]2- 及 [Ben(C4H4)2]Li2 (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[Ben(C4H4)2]2-及[Ben(C4H4)2]Li2 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[Ben(C4H4)2]Li2 (n=2–8)有望通过C4H4Li2/C5H5-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。     

Co(en)3[B4O5(OH)4]Cl·3H2O和[Ni(en)3][B5O6(OH)4]2·2H2O的合成、结构以及热力学性质

利用水热法合成了两种过渡金属配合物为模板剂的含水硼酸盐晶体Co(en)3[B4O5(OH)4]Cl·3H2O(1) 和 [Ni(en)3][B5O6(OH)4]2·2H2O (2),并通过元素分析、X射线单晶衍射、红外光谱及热重分析对其进行了表征。化合物1晶体结构的主要特点是在所有组成Co(en)33+, [B4O5(OH)4]2–, Cl– 和 H2O之间通过O–H…O、O–H…Cl、N–H…Cl和N–H…O四种氢键连接形成网状超分子结构。化合物2晶体结构的特点是[B5O6(OH)4]–阴离子通过O–H…O氢键连接形成沿a方向有较大通道的三维超分子骨架,模板剂[Ni(en)3]2+阳离子和结晶水分子填充在通道中。     

四核Cu(Ⅰ)配合物[Cu4(imdt)9](NO3)4·6H2O的合成与晶体结构

近年来,硫脲类金属配合物在配位化学、生物化学、医药等领域的研究一直受到广泛重视[1,2]。四氢化咪唑-2-硫酮(imdt)又称乙撑硫脲,是乙撑双二硫代氨基甲酸酯类农药的代谢产物。它属于硫酰胺杂环化合物,含—N(H)—C(=S)—=—N=C(—SH)—结构互变活性基团,表现出配位多样性,与金属铜可以形成单核[3]和双核[4,5]配合物。本文合成了四核Cu(I)配合物[Cu4(imdt)9](NO3)4·6H2O,对该配合物进行了元素分析和红外光谱表征,用单晶X-射线衍射测定了晶体结构。1实验部分1·1试剂与仪器配体四氢化咪唑-2硫酮(C3H6N2S,imdt)按文献合成[6],其它药品…     

5-(3-吡啶基)-1H-四氮唑配体构筑的[Ni_2(ptzH)_3(H_2O)_6]~(4+)二聚体修饰的八钼酸盐化合物

在水热条件下采用5-(3-吡啶基)-1H-四氮唑配体合成了基于八钼酸盐的有机-无机杂化化合物[Ni_2(ptz H)_3(H_2O)_6](β-Mo_8O_(26))·2H_2O(ptz H=5-(3-吡啶基)-1H-四氮唑),并通过单晶X-射线、元素分析和红外光谱对其进行了表征.化合物中存在β型八钼酸盐[Mo_8O_(26)]~)4-_和阳离子二聚体[Ni_2(ptz H)_3(H_2O)_6]~(4+)2个孤立的亚单元.在这个二聚体中,2个Ni原子被3个ptz H分子固定.相邻的Ni二聚体之间存在丰富的π…π堆积作用,形成1个带有菱形格子的二维超分子金属-有机层.[β-Mo_8O_(26)]~(4-)多阴离子通过提供大量的氢键作用而占据在该超分子二维层的菱形格子中.     

氨基酸功能化Dawson型多阴离子[P_2Mo_(18)O_(62)]~(6-)化合物的合成及表征

在常规条件下,以质子化的L,D-组氨酸修饰Dawson型多阴离子[P2Mo18O62]6-,得到了一对新型的氨基酸功能化的多金属氧酸盐化合物:H4(L-HC6H9N3O2)2[P2Mo18O62].20.5H2O(1),H4(D-HC6H9N3O2)2[P2Mo18O62].20.5H2O(2).并用单晶X射线衍射,紫外光谱(UV),红外光谱(IR),元素分析(Elemental Analysis)等方法对化合物进行了表征.     

四-(对-磺基苯基)卟啉二酸(H_4~(2+)TSPP)分子聚集体的共振喇曼光谱研究

研究了四－（对－磺基苯基）卟啉二酸（Ｈ２＋４ＴＳＰＰ）的Ｊ－聚集体共振喇曼光谱,用氘代法考察了各喇曼谱带的同位素位移．指认３条低波数喇曼带为分子聚集体的晶格模．喇曼光谱退偏比测量表明,聚集体中Ｈ２＋４ＴＳＰＰ的对称性较分子态降低．比较游离碱Ｈ２ＴＳＰＰ和分子态Ｈ２＋４ＴＳＰＰ共振喇曼光谱讨论了聚集体中Ｈ２＋４ＴＳＰＰ的结构变化．Ｈ２＋４ＴＳＰＰ在聚集体中以接近面对面方式排列     

The influence of aggregation of porphyrins on the efficiency of photogeneration of hydrogen peroxide in aqueous solution

The pH-dependence of the ability of coproporphyrin (CP) and uroporphyrin (UP) to photogenerate hydrogen peroxide (H2O2) in aqueous solution was investigated, with special attention to the structure-activity relationship related to the aggregation of the porphyrins. It was found that the efficiency was strongly dependent on the aggregation of CP and UP mediated by changes in the pH of the solution, and a dimeric form had a weak ability to produce H2O2, while a highly aggregated form had a good ability. The increased efficiency of the highly aggregated porphyrin to produce H2O2 was further demonstrated using a different type of aggregate formed by the electrostatic interaction of cationic tetrakis-5,10,15,20-(N-methyl-4-pyridyl)porphin (TMPyP) with anionic tetrakis-5,10,15,20-(4-sulfonatophenyl)porphin (TSPP). The present results demonstrated the importance of the state of aggregation of porphyrin to photogenerate H2O2, and the results may help to develop a new type of medicine for photodynamic therapy.     

Spectroscopic study of J aggregates of amphiphilic merocyanine dyes formed in their pure Langmuir films

It is known that an amphiphilic merocyanine dye, 3-carboxymethyl-5-[2-(3-octadecyl-2(3H)- benzothiazolylidene)ethylidene]-2-thioxo-4-thiazolidinone (DS) and its derivatives DSe and 6MeDS form J aggregates under the presence of metallic cations, although the dyes' static dipole moments must be favorable for H aggregates. A metal-free J aggregate of 6MeDS has been generated in its pure Langmuir films and transferred onto CaF2 substrates to investigate the molecular environment around the carboxylic group born by the dye. Combining visible and infrared spectroscopy, geometrical consideration based on ab initio calculations, and simulation of the excitation energy, a structural model of this J aggregate has been proposed. With this model, formation of intermolecular carboxyl-keto hydrogen bonds, which can compensate the electrostatic disadvantage of the J aggregate under the presence of water, has been suggested. As for another derivative of DS, DO, similar discussion has been made for its Mg2+ -containing J aggregate, which is found in this work. In addition, the proposed structural model can tell the cause of the difference in the tendency to J aggregate among 6MeDS, DSe, DS, and DO.     

卟啉H2TSPP和Ag(II)TSPP吸附在均分散Fe3O4胶体上的拉曼光谱

Surface Enhanced Raman Scattering (SERS) of tetrasodium meso-tetrakis (4-sulfonatophenyl) porphine (H2TSPP) and silver tetraphenylporphyrin (Ag(Ⅱ)TSPP) adsorbed spontaneously on uniform Fe3O4 colloids are recorded. The enhancement of Raman bands is approximately 30. An analysis of the SERS spectrum shows that on the Fe3O4 surface H2TSPP takes its diacid form H42+TSPP.     

四-(对-磺基苯基)卟啉二酸(H2+4TSPP) 分子聚集体的共振喇曼光谱研究

研究了四-(对-磺基苯基)卟啉二酸(H     

Electrolyte-induced mesoscopic aggregation of thiacarbocyanine dye in aqueous solution: counterion size specificity

Countercation size specificity is presented for the electrolyte-induced aggregation of 3,3'-disulfopropyl-5,5'-dichloro-9-methyl thiacarbocyanine (TCC) dye in aqueous solution. Addition of electrolytes having a small monovalent cation (Na+, NH4+, or Cs+) induced pure H aggregates of TCC, whereas J aggregates were preferentially promoted by electrolytes with a large monovalent cation ([N(CH3)4]+ or [N(C2H5)4]+). The electrolyte-induced H aggregate (HS aggregate) differed spectroscopically from that spontaneously self-assembled in aqueous solution. Mesoscopic structure of the HS aggregates was revealed via polarized-light microscopy and atomic force microscopy; a rodlike morphology of 50-70 nm wide and tens to hundreds of micrometers long with very strong negative birefringence. A simple structural model based on semiempirical molecular orbital calculations can explain the aggregation behaviors: The anionic TCC monomer shows a considerable planar geometry between two benzothiazole end groups when it involves a sodium cation, which favors the H-type molecular arrangements in a face-to-face orientation. On the other hand, the TCC dye has a twisted conformation when it implicates a large tetramethylammonium cation, resulting in the formation of the J aggregates.     

Photoinduced electron transfer from tetrasulfonated porphyrin to benzoquinone revisited. The structural volume-normalized entropy change correlates with marcus reorganization energy

Time-resolved laser-induced optoacoustic spectroscopy was used for the determination of the enthalpy, DeltaTH, and structural volume changes, DeltaTV, concomitant with triplet state formation upon excitation of meso-tetrakis(4-sulfonatophenyl)porphyrin, TSPP(4-), as well as with the triplet state electron-transfer (ET) quenching by benzoquinone, BQ (DeltaRH and DeltaRV). The values of DeltaTH and DeltaTV for (3)TSPP(4-) formation in the presence of different cations (Li+, Na+, K+, NH4+, and Cs+) correlated with each other and afforded a value of DeltaTG = 140 +/- 20 kJ mol(-1), equal to the value of E+ at 77 K, but much larger than the DeltaTH values in solution at room temperature, due to the large entropic factor in solution. The influence of the cations on DeltaTH and DeltaTV (a contraction ranging from 5.4 to 3.8 cm3 mol(-1)) is attributed to changing chromophore-water interactions in the ground and triplet states. Upon quenching of 3TSPP(4-) by BQ, the quantum yield of free radical formation, PhiR = 0.66 +/- 0.04, is the same in the solutions of the five cations. The values of DeltaRH and DeltaRV are small and have a large error. The energy level of the free radicals formed is thus very similar to that of 3TSPP(4-). TDeltaRS and X = TDeltaRS/DeltaRV, i.e., the structural volume change-normalized entropy change for free radicals formation, were derived using average values of DeltaRH and DeltaRV together with the calculated DeltaRG degrees . The measured Marcus reorganization energy, lambda, and X fall into the lambda vs X linear dependence we previously found for the radical formation upon ET quenching of triplet flavins (3FMN and 3FAD) by amines and amino acids. Thus, X = TDeltaRS/DeltaRV in aqueous solutions is a property of the particular donor-acceptor pair linearly correlated to the corresponding Marcus reorganization energy. The value of X is much larger than the predicted value applying the electrostriction concepts in view of the noncontinuum nature of the aqueous solutions.     

Homogeneously mixed porphyrin J-aggregates with rod-shaped nanostructures via zwitterionic self-assembly

To tailor functional nanomaterials, the co-assembly of self-assembling dyes in a homogeneous way would be a promising approach because the electronic properties can be tuned by the mixing ratio. Although porphyrins are important supramolecular building blocks with unique optical properties, a homogeneously mixed J-aggregate system of porphyrins has not been reported yet. Herein, we focused on three kinds of zwitterionic porphyrin diacids, H(4)TSPP(2-), H(4)T(5-STh)P(2-) and H(4)T(4-STh)P(2-), due to their capability to form J-aggregates with distinguished optical properties and well-defined nanostructures. In this study, we investigated the co-assembly behaviours of the zwitterionic porphyrins in aqueous solution by UV-vis and RLS, and investigated the morphology of the resultant homogeneously mixed J-aggregates by AFM. In the case of the combination of H(4)TSPP(2-) and H(4)T(5-STh)P(2-), they readily co-assemble to form homogeneously mixed J-aggregates with different types of binary excitonic bands, whereas the combination of H(4)T(4-STh)P(2-) and other porphyrins results in the dominant formation of the individual pure J-aggregates. Deposited homogeneously mixed J-aggregates of H(4)TSPP(2-) with H(4)T(5-STh)P(2-) consist of rod-shaped nanostructures, whose height changes discontinuously upon varying the mixing ratio. These results would provide new insights into the electronic properties and the nanostructure of self-assembled multicomponent materials.     

Fabrication of CuO pricky microspheres with tunable size by a simple solution route

A simple aqueous solution route was introduced for the fabrication of CuO pricky microspheres (CPMs) using CuCl(2) x 2H(2)O, Na(2)(C(4)H(4)O(6)) x 3H(2)O and NaOH as starting materials. The CPMs were composed of compressed nanothorns exhibiting tapering feature with tip size of less than 10 nm, and the size of CPMs could be tuned from 100-200 nm to 4-6 microm. The effects of the molar ratios of tartrate anions and NaOH to Cu(2+) cations, reagent concentration, and reaction temperature on the products were investigated, showing that the morphology of CPMs was determined by the molar ratio of tartrate to Cu(2+) cations and the size was greatly affected by reagent concentration and the molar ratio of NaOH to Cu(2+) cations in the precursor solution. The fabrication of CPMs went through rapid nucleation of Cu(OH)(2), aggregation and in situ dehydration of Cu(OH)(2), oriented-aggregation-based growth, and normal crystal growth of CuO nanothorns. The nucleation and crystal growth were successfully separated by controlled releasing of Cu(2+) and OH(-) ions through the reversible reaction of Cu(2+) cations, OH(-), and C(4)H(4)O(6)(2-) anions.     

Polyelectrolyte‐Assisted Noncovalent Functionalization of Carbon Nanotubes with Ordered Self‐Assemblies of a Water‐Soluble Porphyrin

The self‐assembly and induced supramolecular chirality of meso‐tetrakis(4‐sulfonatophenyl)porphyrin (TSPP) on both single‐wall (SWCNT) and multiwall carbon nanotubes (MWCNT) are investigated. Under mild pH conditions (pH 3), TSPP forms aggregates when CNTs are dispersed in an aqueous solution containing positively charged polyelectrolytes such as poly‐L ‐lysine (PLL) or poly(allylamine hydrochloride) (PAH). Evidence for the geometry of the porphyrin aggregates is obtained from absorption spectra, whereby the fingerprints of J‐ and H‐aggregates are clearly seen only in the presence of smaller‐diameter nanotubes. J‐aggregates are better stabilized with PLL, whereas in the presence of PAH mainly H‐aggregates prevail. Excited‐state interactions within these nanohybrids are studied by steady‐state and time‐resolved fluorescence. The porphyrin emission intensity in the nanohybrid solution is significantly quenched compared to that of TSPP alone, and this implies strong electronic interaction between CNTs and porphyrin molecules. Fluorescence lifetime imaging microscopy (FLIM) further supports that porphyrin arrays are associated with the MWCNT sidewalls wrapped in PLL. In the case of the SWCNT hybrid, spherical structures associated with longer fluorescence lifetime appeared after one week, indicative of H‐aggregates of TSPP. The latter are the result of π–π stacking of porphyrin units on neighboring nanotubes facilitated by the strong tendency of these nanotubes to interact with each other. These results highlight the importance of optimum dimensions and surface‐area architectures of CNTs in the control/stability of the porphyrin aggregates with promising properties for light harvesting.