2—（2‘—羟基苯基）苯并咪唑的质子转移反应和光谱性质的…

用ＡＭ１和ＩＮＤＯ／Ｓ－ＣＩ方法对２－（２＇－羟基苯基）苯并咪唑的基态和激发态分子内质子转移反应进行了理论研究，求得基态和激发态反应的势能曲线、势垒和过渡态，并研究了此分子的一些异构体、阴离了的相对稳定性，估算了氢键能。进行了实验光谱的理论指认，所得结果与实验值符合较好。在此基础上对光化学反应机理和光谱性质进行了探讨。     

聚丙烯酰胺存在下Mohr法直接滴定碘、银等离子和硫氰酸根

1引言　　　　经典莫尔法对于　０．０１　ｍｏｌ／Ｌ的Ｃｌ－滴定误差达十０．６％需要进行指示剂的空白校正．且因　Ａｇｌ、ＡｇＳＣＮ沉淀强烈吸附Ｉ－和ＳＣＮ－、Ａｇ２ＣｒＯ４。沉淀凝聚后再转化成ＡｇＣｌ极慢，故不适于直接滴定Ｉ－、ＳＣＮ－、Ａｇ－。作者以聚丙烯酰胺（ＰＡＭ）化学修饰ＡｇＸ（ｘ－＝Ｉ－、ＳＣＮ－、Ｂｒ－、Ｃｌ－）及Ａｇ２ＣｒＯ４沉淀的结构，减小Ａｇｘ对Ｘ－的吸附与促进Ａｇ２ＣｒＯ４的转化，用莫尔法直接测定Ｉ－、ＳＣＮ－、Ａｇ＋及不需空白校正能准确滴定　０．０１　ｍｏｌ／ＬＣｌ－未见报道…     

H2C（P（Ph）2AuX）2和HC（P（Ph）2AuX）3（X=I,CI）型配合物的…

根据配合物Ｈ２Ｃ（Ｐ（Ｐｈ）２ＡｕＸ）２（Ｘ＝Ｉ，Ｃｌ）和ＨＣ（Ｐ（Ｐｈ）２ＡｕＸ）３（Ｘ＝Ｉ，Ｃｌ）的晶体结构对它们进行了从头算研究，在ＭＰ２近似水平下得到绕Ｃ－Ｐ旋转所产生构象的势能曲线，从而揭示Ａｕ（Ｉ）－Ａｕ（Ｉ）相互作用，计算结果表明，在所研究的四个配合物中均存在Ａｕ（Ｉ）－Ａｕ（Ｉ）相互作用，该作用较弱，约为１０．０～１６．５ｋＪ／ｍｏｌ，与Ｓｃｈｍｉｂａｕｒ的实验估计值和Ｐｙｙｋｋｏ     

SMAI和CI法制备的Ni—Ag／SiO2催化剂的结构与催化性质研究

应用溶剂化金属原子浸渍（ＳＭＡＩ）法和普通浸渍（ＣＩ）法制备了金属含量相同的ＳｉＯ２负载Ｎｉ－Ａｇ双金属催化剂。ＸＲＤ和磁测定结果表明ＳＭＡＩ催化剂中Ｎｉ和Ａｇ的粒度均小于金属含量相同的ＣＩ催化剂，ＳＭＡＩ催化剂中Ｎｉ和Ａｇ未形成合金，而ＣＩ催化剂中Ｎｉ和Ａｇ形成了合金。ＳＭＡＩ和ＣＩ催化剂都具有超顺磁性。研究了这些催化剂在甲苯加氢反应的催化性质，结果表明与组成相同的普通浸渍法催化相比，ＳＭＡＩ催     

ICP－AES间接法连续测定混合物中的氯和碘离子的研究

本文研究了在Ｃｌ￣－和Ｉ￣－的混合物中，加入过量Ａｇ￣＋使Ｃｌ￣－和Ｉ￣－分别以ＡｇＣｌ和ＡｇＩ沉淀后，用ＩＣＰ－ＡＥＳ测定剩余的Ａｇ￣＋，然后用ＮＨ＿３·Ｈ＿２Ｏ溶解ＡｇＣｌ沉淀，测定溶解液中的Ａｇ￣＋，间接得到Ｃｌ￣－的含量，以差减法求得Ｉ￣－量，实现Ｃｌ￣－和Ｉ￣－的间接法连续测定。本文探讨了有关的化学条件和光谱测定条件，对方法的适用性进行了考察──共存离子的干扰情况，方法的精密度、检出限和试样中加入回收试验。回收率为９７．１％～１０１．２％（Ｃｌ￣－），９８．１％～１００．４％（Ｉ￣－）。     

A FACILE TOTAL SYNTHESIS OF (±)-SELINA-3,11-DIEN-9-OL

Ａ　ＦＡＣＩＬＥ　ＴＯＴＡＬ　ＳＹＮＴＨＥＳＩＳ　ＯＦ　（±）－ＳＥＬＩＮＡ－３，　１１－ＤＩＥＮ－９－ＯＬＡＦＡＣＩＬＥＴＯＴＡＬＳＹＮＴＨＥＳＩＳＯＦ（±）－ＳＥＬＩＮＡ－３，１１－ＤＩＥＮ－９－ＯＬＬｉＪｕｎＬＩＵ；ＺｈａｏＭｉｎｇＸＩＯＮＧ；...     

快原子轰击和电喷雾电离质谱表征烷基苯磺酸盐

用负离子化快原子轰击（ＦＡＢ）和电喷雾电离（ＥＳＩ）质谱并结合碰撞活化解离（ＣＡＤ）质谱方法对烷基苯磺酸盐（ＡＢＳ）进行鉴定。试样在负离子电喷雾电离（ＥＳＩ）过程中不产生碎片峰,但是在ＦＡＢ过程中产生许多碎片、比较这些谱图,就可以区别碎片峰和分子离子峰。线性或支化烷基苯磺酸盐的结构与相对含量可以在离子ＥＳＩ／ＣＡＤ－ＭＳ方法中得到。负离子ＥＳＩ－ＭＳ是快速、有效和可靠的鉴定ＡＢＳ的方法。     

溶剂化金属原子浸渍法制备的Ni－Ag／γ－Al_2O_3催化剂的结构表征

应用溶剂化金属原子浸渍（ＳＭＡＩ）法和普通浸渍（ＣＩ）法制备了三种不同摩尔比的γ－Ａｌ２Ｏ３负载Ｎｉ－Ａｇ双金属催化剂。ＸＲＤ和磁测定结果表明ＳＭＡＩ催化剂中Ｎｉ和Ａｇ的粒度均小于金属含量相同的ＣＩ催化剂，ＳＭＡＩ催化剂中Ｎｉ和Ａｇ未形成合金，而ＣＩ催化剂中Ｎｉ和Ａｇ形成了合金。ＳＭＡＩ和ＣＩ催化剂都具有超顺磁性。ＸＰＳ测定结果表明ＳＭＡＩ催化剂中零价Ｎｉ和Ａｇ的含量均高于ＣＩ催化剂。ＳＭＡＩ催化剂Ｎｉ在表面含量高于体相，Ｎｉ在表面富集，而ＣＩ催化剂Ｎｉ在表面和体相的含量相同     

乙烯系自由基聚合阻聚效应（ⅩⅧ）：哌啶氮氧自由基氨基硫…

本文研究了３种１－（芳酰基）－４［４＇－（２，２，６，６－四甲基哌啶）－１－氧自由基］氨基硫脲化合物（ＡＴＳＣＰＯ）分别同通用阻聚剂（ＣＩＨ），如对苯二酚（ＨＱ），苯醌（ＢＱ），吩噻嗪（ＰＴ）及二乙羟胺（ＤＥＨＡ）组成的混合阻聚剂对ＡＩＢＮ引发的ＭＭＡ自由基聚合的影响，研究结果表明：当［ＡＴＳＣＰＰ］／ＣＩＨ＝５：１时，除ＡＴＳＣＰＯ－ＢＱ外，其余阻聚效果均较ＡＴＳＣＰＯ和ＣＩＨ单独用作阻聚剂时高     

ASYMMETRIC MICHAEL－TYPE ALKYLATION OF CHIRAL IMINES DIASTEREOSELECTIVE SYNTHESIS OF（＋）－α－CYPERONE AND （－）－10－EPI－α－CYPERONE

ＡＳＹＭＭＥＴＲＩＣ　ＭＩＣＨＡＥＬ－ＴＹＰＥ　ＡＬＫＹＬＡＴＩＯＮ　ＯＦ　ＣＨＩＲＡＬ　ＩＭＩＮＥＳ　ＤＩＡＳＴＥＲＥＯＳＥＬＥＣＴＩＶＥ　ＳＹＮＴＨＥＳＩＳ　ＯＦ（＋）－α－ＣＹＰＥＲＯＮＥ　ＡＮＤ　（－）－１０－ＥＰＩ－α－ＣＹＰＥＲＯＮＥＡＳ...     

AsH3 ultraviolet photochemistry: an ab initio view

Multireference configuration interaction calculations have been carried out for low-lying electronic states of AsH(3). Bending potentials for the nine lowest states of AsH(3) are obtained in C(3v) symmetry for As-H distances fixed at the ground state equilibrium value of 2.850 a(0), as well as for the minimum energy path constrained to R(1) = R(2) = R(3). The calculated equilibrium geometry and bond energy for the X (1)A(1) ground state agree very well with the previous experimental and theoretical data. It is shown that the lowest excited singlet state belongs to the (1)A(1) symmetry (in C(3v)), in contradiction to the previous calculations. This state is characterized by a planar equilibrium geometry. Asymmetric stretch potential energy surface (PES) cuts along the H(2)As-H recoil coordinate (at R(1) = R(2) = 2.850 a(0), θ = 123.9° and 90°) for numerous excited states and two-dimensional PESs for the X and ? states up to the dissociation limits are obtained for the first time. The ? (1)A(1), B(1)E-X (1)A(1) transition moments are calculated as well and used together with the PES data for the analysis of possible photodecay channels of arsine in its first absorption band.     

Ab initio molecular orbital study of ground and low-lying electronic states of CoCN

The ground and low-lying excited states of CoCN have been studied by ab initio multireference single and double excitation configuration interaction (MR-SDCI) calculations with Davidson's correction Q and Cowan-Griffin's relativistic corrections. The electronic ground state of CoCN is (3)Phi(i) and the equilibrium geometry is linear with bond lengths of r(e)(Co-C)=1.8540 A and r(e)(C-N)=1.1677 A, substantially different from the experimentally derived values of r(0)(Co-C)=1.8827(7) A and r(0)(C-N)=1.1313(10) A. The first excited state is (3)Delta(i), separated from the ground state by 727 cm(-1). Larger dynamical electron correlation energy for the low-spin (3)Phi state than for the high-spin (5)Phi state makes the (3)Phi state to be the ground state, which is discussed in terms of the differences in natural orbitals. A new spin-orbit interaction scheme between the X (3)Phi(i) and 1 (3)Delta(i) states is proposed.     

Theoretical investigation of excited states of C(3)

In this work, we present ab initio calculations for the potential energy surfaces of C(3) in different electronic configurations, including the singlet ground state [X (1)Sigma(g) (+),((1)A(1))], the triplet ground state [a (3)Pi(u),((3)B(1), (3)A(1))], and some higher excited states. The geometries studied include triangular shapes with two identical bond lengths, but different bond angles between them. For the singlet and triplet ground states in the linear geometry, the total energies resulting from the mixed density functional--Hartree-Fock and quadratic configuration interaction methods reproduce the experimental values, i.e., the triplet occurs 2.1 eV above the singlet. In the geometry of an equilateral triangle, we find a low-lying triplet state with an energy of only 0.8 eV above the energy of the singlet in the linear configuration, so that the triangular geometry yields the lowest excited state of C(3). For the higher excited states up to about 8 eV above the ground state, we apply time-dependent density functional theory. Even though the systematic error produced by this approach is of the order of 0.4 eV, the results give different prospective to insight into the potential energy landscape for higher excitation energies.     

The o-, m-, and p-benzyne radical cations: a theoretical study

On the basis of the CASPT2 (multiconfigurational second-order perturbation theory) geometry optimization calculations, the ground states of the o-C(6)H(4)(+) (C(2v)), m-C(6)H(4)(+) (C(2v)), and p-C(6)H(4)(+) (D(2h)) radical cations were determined to be 1 (2)B(1), 1 (2)A(2), and 1 (2)B(1u), respectively. For o-C(6)H(4)(+) and m-C(6)H(4)(+), the first excited states (1 (2)A(2) and 1 (2)A(1), respectively) lie very close to the respective ground states. The small distance value of 1.419 A between the two dehydrocarbons in the ground-state geometry of m-C(6)H(4)(+) indicates that there is a real chemical bond between the two dehydrocarbons (the distance in the 1 (2)A(1) geometry of m-C(6)H(4)(+) is very long as in the m-C(6)H(4) molecule). The (U)B3LYP isotropic proton hfcc (hyperfine coupling constant) calculation results imply that the ground and first excited states of o-C(6)H(4)(+) will have similar ESR spectrum patterns while the ground and first excited states of m-C(6)H(4)(+) will have completely different ESR spectrum patterns.     

Dibenzo-p-dioxin. An ab initio CASSCF/CASPT2 study of the pi-pi* and n-pi* valence excited states

The pi-pi* and n-pi* valence excited states of dibenzo-p-dioxin (DD) were studied via the complete active space SCF and multiconfigurational second-order perturbation theory employing the cc-pVDZ basis set and the full pi-electron active spaces of 16 electrons in 14 active orbitals. The geometry and harmonic vibrational wavenumbers of the ground state correlate well with the experimental and other theoretical data. In particular, significant improvements over previously reported theoretical results are observed for the excitation energies. All of the pi-pi* excited states exhibit planar D(2h)minima. Thus no evidence was found for a C(2v) butterfly-like relaxation, although the wavenumbers of the b(3u) butterfly flapping mode proved exceedingly low in both the ground S(0)((1)A(g)) and the lowest dipole allowed excited S(1)((1)B(2u)) state. The calculations of oscillator strengths established the 2(1)B(2u) <-- 1(1)A(g) and 2(1)B(1u) <-- 1(1)A(g) transitions as by far the most intense, whereas the only allowed of the n-pi* transitions ((1)B(3u)) should possess only a modest intensity. Studies into dependence of the oscillator strengths on the extent of the butterfly-like folding showed that the electronic spectrum is more consistent with a folded equilibrium geometry assumed by DD in solution.     

Electronic structures of low-lying Bu excited states in trans-oligoenes: Pariser-Parr-Pople and ab initio calculations

Two lowest-lying excited singlets with B(u) symmetry of all-trans-oligoenes, the well-known ionic 1(1)B(u)(+) state as well as the "hidden" ionic-covalent-mixed 1(1)B(u)(-) state, are calculated within both the Pariser-Parr-Pople (PPP) model at full configuration interaction (FCI) level and ab initio methods. The vertical excitation energies as well as wavefunctions from PPP-FCI calculations are found to be in good agreement with those from high-level multi-reference methods, such as multi-reference complete active space self-consistent field (CASSCF) with second order perturbative corrections (CASPT2), multi-reference M?ller-Plesset perturbation theory (MRMP), and complete active space valence bond theory (CASVB). The oscillator strengths from PPP calculation are in good agreement with spectroscopy experiments. The relatively small oscillator strength of 1(1)B(u)(-) is due to the approximate electron-hole symmetry of this state. In addition, the bond lengths in both states are found to show remarkable relativity with the bond orders calculated with ground state geometries, which suggests a possible strategy for initial guess in geometry optimization of excited states.     

Conformation and intramolecular hydrogen bonding of 2-chloroacetamide as studied by microwave spectroscopy and quantum chemical calculations

The microwave spectrum of 2-chloroacetamide (ClCH2CONH2) has been investigated at room temperature in the 19-80 spectral range. Spectra of the 35ClCH2CONH2 and 37ClCH2CONH2 isotopomers of one conformer, which has a symmetry plane (Cs symmetry), were assigned. The amide group is planar, and an intramolecular hydrogen bond is formed between the chlorine atom and the nearest hydrogen atom of the amide group. The ground vibrational state, six vibrationally excited states of the torsional vibration about the CC bond, as well as the first excited state of the lowest bending mode were assigned for the 35ClCH2CONH2 isotopomer, whereas the ground vibrational state of 37ClCH2CONH2 was assigned. The CC torsional fundamental vibration has a frequency of 62(10) cm(-1), and the bending vibration has a frequency of 204(30) cm(-1). The rotational constants of the ground and of the six excited states of the CC torsion were fitted to the potential function Vz = 16.1( + 2.3) cm(-1), where z is a dimensionless parameter. This function indicates that the equilibrium conformation has Cs symmetry. Rough values of the chlorine nuclear quadrupole coupling constants were derived as chi(aa) = -47.62(52) and chi(bb) = 8.22(66) MHz for the 35Cl nucleus and chi(aa) = -34.6(10) and chi(bb) = 6.2(11) MHz for the 37Cl nucleus. Ab initio and density functional theory quantum chemical calculations have been performed at several levels of theory to evaluate the equilibrium geometry of this compound. The density functional theory calculations at the B3LYP/6-311++G(3df,2pd) and B3LYP/cc-pVTZ levels of theory as well as ab initio calculations at the MP2(F)/cc-pVTZ level predict correct lowest-energy conformation for the molecule, whereas the ab initio calculations at the QCISD(FC)/6-311G(d) and MP2(F)/6-311++G(d,p) levels predict an incorrect equilibrium conformation.     

Multireference configuration interaction studies on the ground and excited states of N2O2: the potential energy curves of N2O2 along N-N distance

In this paper, the ground and excited states of N2O2 were studied at the multireference configuration interaction (MRCI) level of theory with Dunning's [J. Chem. Phys. 90, 1007 (1985); 96, 6796 (1992)] correlation consistent basis sets augo-cc-pVDZ and aug-cc-pVTZ. The geometry optimizations were performed for the ground state of N2O2. The vertical excitation energies and transition moments were calculated for the low-lying singlet states of N2O2 including the lowest three 1A1 states, two 1B1 states, one 1B2 state, and two 1A2 states at the MRCI level of theory with Dunning's correlation consistent basis sets aug-cc-pVDZ, aug-cc-pVTZ, and aug-cc-pVQZ. Furthermore, for the first time, the potential energy curves were calculated at the complete active space self-consistent-field and MRCI levels of theory for as many as 12 N2O2 singlet electronic states along the N-N distance. The dissociation asymptotes of these 12 N2O2 singlet electronic states were discussed.     

Substituent effects on twisted internal charge transfer excited states of N-borylated carbazoles and (diphenylamino)boranes

N-Boryl-substituted carbazoles (carBR(2)) and (diphenylamino)boranes (Ph(2)NBR(2)) with R = Mes (mesityl) and FMes [tris(trifluoromethyl)phenyl] substituents on boron exhibit large UV/vis Stokes shifts. To investigate the substituent effect on the magnitude of the Stokes shifts, we studied the electronic structure and spectroscopic properties of carBR(2) and Ph(2)NBR(2) with R = H, Mes, and FMes using hybrid density functional theory (B3LYP) and time-dependent density functional theory (TD-B3LYP) for ground and low-lying excited states. The lowest lying excited state with a nonvanishing oscillator strength is a twisted internal charge transfer (TICT) (1)A state in the C(2) point group, owing to a single-electron excitation from the nitrogen lone pair to the unoccupied boron p(z) AO, Nlp → Bp(z). Emission from these (1)A excited states are predicted to be much brighter than from the energetically close (1)B excited states that are not directly related to CT excitation from N to B, due to symmetry. An analysis of geometrical relaxations in the excited state and the state energies relative to the ground state energy of the equilibrium geometry reveals that (a) the carbazole skeleton induces a general red shift in UV/vis spectra, (b) bulky boryl substituents reduce the predicted Stokes shifts of TICT states, and (c) the presence of electron-withdrawing functional groups induces a further general red shift in UV/vis spectra but does not significantly alter Stokes shifts.     

The low-lying electronic excited states of NiCO

Highly correlated coupled cluster methods with single and double excitations (CSSD) and CCSD with perturbative triple excitations were used to predict molecular structures and harmonic vibrational frequencies for the electronic ground state X 1Sigma+, and for the 3Delta, 3Sigma+, 3Phi, 1 3Pi, 2 3Pi, 1Sigma+, 1Delta, and 1Pi excited states of NiCO. The X 1Sigma+ ground state's geometry is for the first time compared with the recently determined experimental structure. The adiabatic excitation energies, vertical excitation energies, and dissociation energies of these excited states are predicted. The importance of pi and sigma bonding for the Ni-C bond is discussed based on the structures of excited states.