Two-Photon Absorption and Excited-State Refractions in Anthraquinone Dyes

We examine the nonlinear optical properties of solutions of 9,10-anthraquinone, 1,4-dihydroxy-anthraquinone, 5,8-dichloro-1,4-dihydroxy-anthraquinone and 1,4-bisethylamino-anthraquinone by means of the intensity-dependent transmission and the Z-scan method with 532 nm 8 ns pulses. The results demonstrated that the 9,10-anthraquinone displayed a two-photon absorption (TPA) character. The molecular TPA cross section of this compound is estimated as σ₂ = 7.22 × 10^?19 cm⁴/GW or σ₂ = 26.96 × 10^?48 cm⁴/photon/s, respectively, and an essential state of ‘m¹Ag’, which should be located near the 2ω virtual transition state, is predicted. On the other hand, the effective excited-state nonlinear refractive coefficients n₂^eff of these anthraquinones are found to be ～10^?10 esu, which are comparable with those highly conjugated planar molecules of tetrabenzporphyrins and phthalocyanines.     

Excited-State Hydrogen Bonding Dynamics of Hydrogen-Bonded Clusters Formed by of Coumarin Derivatives in Aqueous Solution: A Time-Dependent Density Functional Theory Study

The time-dependent density functional theory and the density functional theory are used to investigate the nature of hydrogen bonds formed by the derivative of the coumarin (TFKC) and the water molecules. The ground-state geometry optimizations, electronic excited energies and corresponding oscillation strengths for the TFKC monomer, the hydrogen-bonded TFKC–Water (HBA) dimer, TFKC–Water (HBB) dimer and TFKC–2Water complex are calculated. We find that, upon photoexcitation, the weaker hydrogen bond in the ground state will be affected by the relatively large impact for TFKC in the water. For better understanding the properties of the hydrogen bonds in the excited states, the frontier molecular orbitals of the S0 and S1 states are shown, and we find the obvious electron density transitions form the water molecules to the TFKC monomer. The electron transfer is expected to be the reason the hydrogen bond dynamics happens.     

Bis(tridentate) Ruthenium-Terpyridine Complexes Featuring Microsecond Excited-State Lifetimes

A series of heteroleptic bis(tridentate) ruthenium(II) complexes, each bearing a substituted 2,2':6',2″-terpyridine (terpy) ligand, is characterized by room temperature microsecond excited-state lifetimes. This observation is a consequence of the strongly σ-donating and weakly π-accepting tridentate carbene ligand, 2',6'-bis(1-mesityl-3-methyl-1,2,3-triazol-4-yl-5-idene)pyridine (C(∧)N(∧)C), adjacent to the terpy maintaining a large separation between the ligand field and metal-to-ligand charge transfer (MLCT) states while also preserving a large (3)MLCT energy. The observed lifetimes are the highest documented lifetimes for unimolecular ruthenium(II) complexes and are four orders in magnitude higher than that associated with [Ru(terpy)(2)](2+).     

Excited-State Double Proton Transfer in 1-Azacarbazole Hydrogen Bonded Complexes

Excited-state double proton transfer (ESDPT) has been studied in a variety of 1-azacarbazole (1AC) hosted hydrogen-bonded complexes. In 1 AC/carboxylic acids hydrogen bonded complexes, large association constants of > 1.0 × 10⁴ M^?1 are measured in the ground state and the rate of ESDPT is » 5.0 × 10⁹ s^?1, resulting in a dominant proton-transfer tautomer emission. In several 1 AC/lactam hydrogen bonded complexes, however, spectral and dynamic results show the existence of a fast excited-state equilibrium between normal and proton-transfer tautomer states. The result can be tentatively rationalized by a non-catalytic ESDPT mechanism incorporating tautomerization energy of the guest molecule.     

Effect of Delocalization and Rigidity in the Acceptor Ligand on MLCT Excited-State Decay

In its most simple form, the energy gap law for excited-state nonradiative decay predicts a linear dependence of ln k(nr) on the ground- to excited-state energy gap, where k(nr) is the rate constant for nonradiative decay. At this level of approximation, the energy gap law has been successfully applied to nonradiative decay in a wide array of MLCT excited states of polypyridyl complexes of Re(I), Ru(II), and Os(II). This relationship also predicts a dependence of k(nr) on the structural characteristics of the acceptor ligand. We report here a brief survey of the literature which suggests that such effects exist and have their origin in the extent of delocalization of the excited electron in the ligand pi framework and on acceptor ligand rigidity.     

窄带系聚合物APFO3的激发态光物理特性

化学计算证实了光致激发窄带系聚合物APFO3后,会发生链内电荷转移（ICT）过程,同时这一特性还影响了吸收光谱中的第一吸收带. 瞬态吸收结果再一次表明了当聚合物在单分散体系中确实存在ICT特性,而且这种特性会同振动弛豫竞争. 在聚集态中,受链间相互作用的影响,ICT特性会消失,而且激子弛豫过程将在光致激发后的弛豫过程中占据主导地位. 混有PC61BM的APFO3薄膜的光致激发动力学显示,当PC61BM 的含量超过50%时,激子解离已经达到饱和. 基于此异质节的光伏器件性能显示PC61BM的含量高于50％以后,光电流的增幅也很小．     

A Spectroscopic Study on Ground- and Excited-State Proton Transfer Reactions of Coumarin Derivatives

Interaction of Coumarin 1, its 3-aldehyde derivative, and biscoumarin with solvents of varying acidity (water and ethanol with an alkali or acid admixture) was studied by following changes in their absorption and luminescence properties. The reasons for weak emission ability of neutral ethanolic solutions of 3-substituted derivatives of Coumarin 1 were revealed.     

水杨酸激发态质子转移反应及其溶剂效应的理论研究

用AMI和INDO/CI方法对水杨酸的激发态质子转移反应进行了理论研究,求得反应的位能曲线、势垒和过渡态,对有关化合物的吸收和荧光光谱进行了理论指认,计算与实验结果符合较好。对光化学反应机理和应用前景进行了讨论,最后以乙醚作为氢键溶剂的例子研究了影响水杨酸激发态质子转移反应的溶剂效应。     

Subpicosecond Excited-State Proton Transfer Preceding Isomerization During the Photorecovery of Photoactive Yellow Protein

The ultrafast excited-state dynamics underlying the receptor state photorecovery is resolved in the M100A mutant of the photoactive yellow protein (PYP) from Halorhodospira halophila. The M100A PYP mutant, with its distinctly slower photocycle than wt PYP, allows isolation of the pB signaling state for study of the photodynamics of the protonated chromophore cis-p-coumaric acid. Transient absorption signals indicate a subpicosecond excited-state proton-transfer reaction in the pB state that results in chromophore deprotonation prior to the cis-trans isomerization required in the photorecovery dynamics of the pG state. Two terminal photoproducts are observed, a blue-absorbing species presumed to be deprotonated trans-p-coumaric acid and an ultraviolet-absorbing protonated photoproduct. These two photoproducts are hypothesized to originate from an equilibrium of open and closed folded forms of the signaling state, I(2) and I(2)'.     

Tetrahedral Carbonylcobalt Clusters

A variety of general methods is available for the synthesis of tetrahedral heteronuclear cobalt clusters of type (CO)₉Co₃E(L)_n (E=hetero element). The size of E has a limiting effect on the existence of such complexes. No compounds (CO)₉Co₃E(L)_n have so far been prepared in which the covalent radius of E exceeds 1.30 Å;. Elements such as In, Sn, Pb, Sb, or Bi do not fit into the tetrahedral Co₃E cluster unit and form open complexes E[Co(CO)₄]_n (n=3, 4). Structural variations among the heteronuclear clusters are encountered in the presence or absence of carbonyl bridges between the cobalt atoms: hetero atoms E bearing several ligands L favor bridging, whereas those bearing only one ligand or none at all permit terminal bonding of all the CO groups.     

多元多金属含氧簇合物

多金属含氧簇合物是一大类具有独特结构和特殊性能的化合物,对于基础理论研究和实际应用均有重要意义,其中多元多金属含氧簇合物的重要性日益渐增,本文拟对多元多金属含氧簇合物的结构,性能和制备作扼要的评述。     

Ligand-Free Metal Clusters

Recent advances in the synthesis and spectroscopic characterization of ligand-free metal clusters immobilized in cryogenic rare gas matrices have contributed greatly to the understanding of electronic, geometric, dynamic, and chemical bonding properties of a wide range of uni- and bimetallic clusters as a function of nuclearity and metal type. The knowledge accumulated on molecular metal aggregates devoid of ligands and isolated on various supports will form an important data base for gauging the reliability of quantum chemical calculations on metal clusters, as well as for comprehending certain aspects of chemisorption on, and catalysis by, supported metal clusters. It can be envisaged that information on ligand-free metal clusters entrapped in a wide range of matrix environments in conjunction with the data for these same metal clusters in the gas phase and in molecular beams will probably contribute towards understanding metal-support interactions and to the designed synthesis of a new breed of high-technology heterogeneous catalysts in the not too distant future.     

Excited-State Electronic Structure with Configuration Interaction Singles and Tamm-Dancoff Time-Dependent Density Functional Theory on Graphical Processing Units

Excited-state calculations are implemented in a development version of the GPU-based TeraChem software package using the configuration interaction singles (CIS) and adiabatic linear response Tamm-Dancoff time-dependent density functional theory (TDA-TDDFT) methods. The speedup of the CIS and TDDFT methods using GPU-based electron repulsion integrals and density functional quadrature integration allows full ab initio excited-state calculations on molecules of unprecedented size. CIS/6-31G and TD-BLYP/6-31G benchmark timings are presented for a range of systems, including four generations of oligothiophene dendrimers, photoactive yellow protein (PYP), and the PYP chromophore solvated with 900 quantum mechanical water molecules. The effects of double and single precision integration are discussed, and mixed precision GPU integration is shown to give extremely good numerical accuracy for both CIS and TDDFT excitation energies (excitation energies within 0.0005 eV of extended double precision CPU results).     

Remarkable Anticancer Activity of Triruthenium-Arene Clusters Compared to Tetraruthenium-Arene Clusters

Abstract The in vitro activity of a series of ruthenium clusters, [(η⁶-C₆H₆)(η⁶-C₆Me₆)₂Ru₃(μ-H)₃(μ₃-O)][BF₄], [(η⁶-C₆H₆)(η⁶-1,4-ⁱPrC₆H₄Me)(η⁶-C₆Me₆)Ru₃(μ-H)₃(μ₃-O)][BF₄], [(η⁶-C₆H₆)₄Ru₄(μ-H)₄][BF₄]₂, [(η⁶-C₆H₅Me)₄Ru₄(μ-H)₄][BF₄]₂ and [(η⁶-C₆H₆)₄Ru₄(μ-H)₃(μ-OH)][Cl]₂, has been evaluated against A2780 and A2780cisR ovarian carcinoma cell lines. Both triruthenium clusters are very active compared to ruthenium compounds in general, whereas the tetraruthenium clusters do not display significant cytotoxicities. Since the triruthenium clusters are known to form supramolecular interactions with arenes and other functions, it is possible that such interactions are also important with respect to their mode of biological activity. The X-ray structure analysis of [(η⁶-C₆H₅Me)₄Ru₄(μ-H)₄][PF₆]₂ is also reported. Graphical Abstract The in vitro activity of a series of ruthenium clusters has been evaluated against A2780 and A2780cisR ovarian carcinoma cell lines and their activity compared to cisplatin. The triruthenium clusters are very active, while the tetraruthenium clusters do not display significant cytotoxicities. Dedicated to Professor Dieter Fenske on the occasion of his 65th birthday anniversary     

Condensed Metal Clusters

The chemistry of metals in low valence states is marked by the frequent occurrence of metal clusters, which are easily recognizable when they occur as molecular units. Many metal-rich compounds of transition metals with p-elements (3rd to the 6th main groups) are closely related to the corresponding halides, since they are built up from metal clusters of the same type. The clusters are however, linked together (condensed) by metal-metal bonds. This principle of construction holds particularly well in the case of the novel reduced halides of the lanthanoids.     

Octanuclear Rare-Earth Clusters

The polyoxo rare-earth core (Ln = Y, Gd, and Yb) has been synthesized from the appropriate rare-earth chloride hydrate and K₂Se and Se in dmf (dimethylformamide). The cluster core is ligated with a variety of polyselenido chains in addition to a number of dmf molecules. The structure of the Gd₈(dmf)₁₃(₄-O)(₃-OH)₁₂(Se₃)(Se₄)₂(Se₅)₂ cluster, 1, was determined by X-ray diffraction methods. It is similar to an Eu cluster previously characterized. Two new clusters, Yb₈(dmf)₁₁(₄-O)(₃-OH)₁₂(Se₄)₂(Se₅)₂Cl₂·dmf, 2, and Y₈(dmf)₁₂(₄-O)(₃-OH)₁₂(Se₄)₄Cl₂·6 dmf, 3, have also been synthesized and characterized. Clusters 2 and 3 have the same octanuclear core of rare-earth atoms as the Gd cluster but contain two chloro ligands in two isomeric conformations in place of the Se ₃ ^2- ring in the Gd cluster. The geometry of the Ln ₈ core is described as a triangulated dodecahedron with ₃-OH groups capping the 12 faces. A ₄-O atom centers the cluster with close contacts to four Ln atoms in an approximate tetrahedral arrangement. Pertinent crystallographic data are: Compound 1, monoclinic, , a= 14.410(3) Å, b = 24.439(5) Å, c = 28.927(6) Å, = 101.05(3)°, V = 9998(3) ų, T = 106(2) K, Z = 4; Compound 2, orthorhombic, , a = 17.049(9) Å, b = 24.68(1) Å, c = 45.03(2)Å, V = 18,945(16) ų, T = 153(2) K, Z = 8; Compound 3, monoclinic, C _2h ⁵ -P2₁/c, a =18.728(l) Å, b = 29.263( 1) Å, c = 20.548(1) Å, = 90.144(1)°, V = 11,261(1) ų, T = 153(2) K, Z = 4.