两种影响生态环境的亚硝基取代烷烃的电子结构

采用紫外光电子能谱实验(PES)和量子化学方法对两种影响生态环境的亚硝基取代烷烃RONO[R=(CH3)2CH,(CH3)3CO]的电子结构进行了分析和讨论。实验得到两种化合物的第一电离能分别为10.37eV和10.12eV,结合从头算自洽场分子轨道(abinitioSCFMO)计算和外壳层格林函数法(OVGF)计算对PES进行了分析和指认。研究表明化合物中取代基效应对电离能存在明显的影响;外层格林函数法计算得到电离能与实验吻合很好;同时发现在外层格林函数计算结果中由于考虑相关能,得到的分子轨道存在能级顺序的交错。实验和理论计算结果进一步证实亚硝基取代烷烃是产生烷基氧自由基(RO^.)的很好的源物种,这为深入研究由它们产生的对环境破坏有着重要影响的相应自由基奠定了基础。     

过渡金属化合物能谱的理论计算

本文提出了在限制Hartree-Fock方法计算的单电子分子轨道基础上计算分子价电子体系能谱和多电子状态的不可约张量方法, 并利用这种方法, 计算了过渡金属化合物CrCl_6~(3-), CrF_6~(3-), CrO_6~(9-), Cr(H_2O)_6~(3+), Cr(NH_3)_6~(3+), Cr(CN)_6~(3-)的d-d跃迁能谱, 计算结果与实验基本符合, 误差一般为1～2 kcm~(-1), 只有个别情况为3.9 kcm~(-1)。     

铂(100)面上CO吸附的量子化学处理

本文用EHMO法对Pt(100)面上CO的吸附进行了处理。先计算了Pt-Pt,Pt-H,Pt-C 等二元体系的平衡间距及离解能,与实测值进行比较以确定计算中所用的基轨道及其轨道参数(如电离电位及轨道指数)以及非对角哈密顿矩阵元的近似方式。然后假设了三种吸附模型,分别进行计算。结果能很好地解释CO在Pt表面上的吸附型式以及 C-O键吸附后减弱的情况,并与红外光谱的实验结果一致。由计算得到的吸附能与由热脱附测得的脱附活化能颇相近。从紫外光电子能谱得到CO分子中σ_(2ρ)轨道的能级吸附后产生位移和π_(2ρ)轨道的能峰重迭。计算的结果表明,CO中的σ_(2ρ)轨道吸附后的稳定化程度确较π_(2ρ)轨道大,因而谱线向π_(2ρ)方向移动。又根据“表面分子”的对称性,对CO和Pt之间的轨道相互作用以及CO在Pt上的解离进行了讨论。     

环芳类化合物紫外光电子能谱的Xα理论研究

本文应用重叠模型多重散射X~α自洽 场方法分析对位环芳([2.2]Paracyclophane)及其氟代化合物(1, 1, 2, 2, 9, 9, 10,10-Octafluoro[2.2]Paracyclophane)和1, 5-Cyclooctadiyne分子的前线分子轨道的相互作用, Through-Space和Through-Bond相互作用对分子能级的影响。考察分子中苯环发生弯曲对分子轨道相互作用的影响, 进一步从过渡态方法计算分子轨道的电离能, 计算结果和实验符合较好, 同时还反映了氟取代后所产生的全氟效应。     

CFCl3的理论和紫外光电子能谱研究

采用紫外光电子能谱(PES)和量子化学方法,研究了以CFCl3化合物为代表的系列化合物(CFCl3、CF2Cl2、CF3Cl、CCl4)不同离子态的电子结构和性质。结果表明,四种化合物CF3Cl、CF2Cl2、CFCl3、CCl4的第一电离能依次下降。结合从头算自洽场分子轨道(abinitioSCFMO)和外壳层格林函数法(OVGF)计算对化合物的PES进行了分析和指认,表明化合物的外层轨道中Cl的孤对电子成分对电离能存在明显的影响;外层格林函数法计算得到电离能与实验吻合很好;同时发现在外壳层格林函数法计算结果中由于考虑相关能,得到的分子轨道存在能级顺序的交错。     

取代环戊二烯基铬-硫三键化合物[η~5-RC_5H_4Cr(CO)_2]_2S的合成、反应及结构

通过η~5-官能团取代环戊二烯基三羰基铬钠与SOCl_2相作用可制得[η~5-CH_3C(O)C_5H_4Cr(CO)_2]_2S1,[η~5-CH_3O_2CC_5H_4Cr(CO)_2]_2S 2和[η~5-C_2H_5O_2CC_5H_4Cr(CO)_2]_2S 3;将1进一步用NaBH_4还原以及2经皂化、酸化和丙酮重结晶制得[η~5-CH_3CH(OH)C_5H_4Cr(CO)_2]_2S 4和[η~5-HO_2CC_5H_4Cr(CO)_2]_2S·nCH_3C(O)CH_3 5.1—5是首次报道的一类含有机官能团的铬-硫三键化合物。1经X射线单晶结构分析表明,它是由一个硫原子通过三键将2个相同的金属有机碎片η~5-CH_3C(O)C_5H_4Cr(CO)_2连在一起的,其Cr≡S≡Cr结构单元呈线性构型,平均Cr≡S三键键长为2.072。     

用同步辐射光研究CO在Cs/Ru(100)表面的吸附

(CO+Cs)/Ru(1010)共吸附的体系中,CO分子由于受CS原子强烈影响,分子轨道发生重新杂化组合.CO分子原来在清洁Ru(1010)表面上结合能位于7.5eV处相重叠的5σ和1π轨道对应谱峰分裂为两峰,结合能分别位于6.3和7.8eV处.其中6.3eV处的谱峰来自CO分子1π轨道的一支,它显示出该分子轨道沿衬底<0001>晶向的镜面反对称性.CO分子1π轨道的另一支和5σ轨道在结合能7.8eV处相重叠.     

过渡金属双核化合物Cr_2(O_2CH)_4、Mo_2(O_2CH)_4及CrMo(O_2CH)_4的从头计算研究

用从头计算方法研究双核过渡金属化合物Cr_2(O_2CH)_4、MO_2(O_2CH)_4及CrMo(O_2CH)_4的金属—金属多重键性质,计算优化键长与实验值符合很好,原子布居表明Mo_2(O_2CH)_4和CrMo(O_2CH)_4中Mo—Mo、Cr—Mo键分别为σ~2π~4δ~2与σ~2δ~2π~4四重键,同时金属-d与氧和碳-p电子间的电荷重叠对分子稳定有相当贡献。对Cr_2(O_2CH)_4在优化键长下3种组态σ~2δ~2δ~(*2)σ~(*2)、π~4π~(*4)及σ~2δ~2π~4的电子结构、原子布居、总能量及电离能的计算进行比较,讨论了Cr—Cr的成键性质,指出描述Cr—Cr间金属多重键本质必须考虑电子相关效应的影响。     

BrCl紫外光电子能谱实验及理论研究

采用紫外光电子能谱研究了影响大气臭氧浓度的重要卤素互化物一氯化溴的精细电离能谱．实验得到BrCl的第一绝热电离能和垂直电离能分别为10．95eV和11．00eV．BrCl的最高占据轨道6π电离产生了明显的旋轨分裂谱带．这对旋轨分裂谱带分别清晰地显示出4个振动精细结构峰．频率分析显示BrCl分子最高占据轨道为弱反键性质．比较了HF方法和外壳层格林函数方法(OVGF)对电离能的计算结果,并对实验值进行了分析比较及指认．采用实验构型OVGF方法给出的电离能结果无论在低电离能区还是在高电离能区都和实验值一致,特别是第一垂直电离能10．988eV与实验值11．00eV非常好地吻合．     

过渡金属化合物的CNDO计算IV——络合物M(CO)_4~(n-)和 M(N_2)_4~(n-)的电子结构

本文对 CNDO(sp-d)方案作了新的改进,改进的要点是把过渡金属原子基函数区分成 s、p、d 三类轨道,据此选择了相应的参数.在 TQ-16机上已实现ALGOL 语言程序.文中报导了 M(CO)_4~(n-)和 M(N_2)_4~(n-)(M=Ni,Co,Fe)电子结构的计算结果,讨论了各 MO 的组成,并结合计算的 Mulliken 和 Wiberg 键序数值讨论了络离子的γ_(MC)及γ_(CO)规律.基于计算的分子轨道能级对 Ni(CO)_4的光电子能谱进行了指定.     

Bonding in a borylene complex investigated by photoionization and dissociative photoionization

The borylene complex [(OC)(5)Cr=B=N(SiMe(3))(2)] has been investigated by using threshold photoelectron-photoion coincidence spectroscopy with synchrotron radiation. The ionization energy of the parent complex and the 0?K appearance energies of the sequential CO loss channels have been determined. The derived bond-dissociation energies are used to discuss bonding and energetics in this compound.     

Spectroscopic detection and theoretical confirmation of the role of Cr2(CO)5(C5R5)2 and .Cr(CO)2(ketene)(C5R5) as intermediates in carbonylation of N=N=CHSiMe3 to O=C=CHSiMe3 by .Cr(CO)3(C5R5) (R = H, CH3)

Conversion of N=N=CHSiMe3 to O=C=CHSiMe3 by the radical complexes .Cr(CO)3C5R5 (R = H, CH3) derived from dissociation of [Cr(CO)3(C5R5)]2 have been investigated under CO, Ar, and N2 atmospheres. Under an Ar or N2 atmosphere the reaction is stoichiometric and produces the Cr[triple bond]Cr triply bonded complex [Cr(CO)2(C5R5)]2. Under a CO atmosphere regeneration of [Cr(CO)3(C5R5)]2 (R = H, CH3) occurs competitively and conversion of diazo to ketene occurs catalytically as well as stoichiometrically. Two key intermediates in the reaction, .Cr(CO)2(ketene)(C5R5) and Cr2(CO)5(C5R5)2 have been detected spectroscopically. The complex .Cr(13CO)2(O=13C=CHSiMe3)(C5Me5) has been studied by electron spin resonance spectroscopy in toluene solution: g(iso) = 2.007; A(53Cr) = 125 MHz; A(13CO) = 22.5 MHz; A(O=13C=CHSiMe3) = 12.0 MHz. The complex Cr2(CO)5(C5H5)2, generated in situ, does not show a signal in its 1H NMR and reacts relatively slowly with CO. It is proposed to be a ground-state triplet in keeping with predictions based on high level density functional theory (DFT) studies. Computed vibrational frequencies are also in good agreement with experimental data. The rates of CO loss from 3Cr2(CO)5(C5H5)2 producing 1[Cr(CO)2(C5H5)]2 and CO addition to 3Cr2(CO)5(C5H5)2 producing 1[Cr(CO)3(C5H5)]2 have been measured by kinetics and show DeltaH approximately equal 23 kcal mol(-1) for both processes. Enthalpies of reduction by Na/Hg under CO atmosphere of [Cr(CO)n(C5H5)]2 (n = 2,3) have been measured by solution calorimetry and provide data for estimation of the Cr[triple bond]Cr bond strength in [Cr(CO)2(C5H5)]2 as 72 kcal mol(-1). The complex [Cr(CO)2(C5H5)]2 does not readily undergo 13CO exchange at room temperature or 50 degrees C implying that 3Cr2(CO)5(C5H5)2 is not readily accessed from the thermodynamically stable complex [Cr(CO)2(C5H5)]2. A detailed mechanism for metalloradical based conversion of diazo and CO to ketene and N2 is proposed on the basis of a combination of experimental and theoretical data.     

From strong van der Waals complexes to hydrogen bonding: From CO⋯H2O to CS⋯H2O and SiO⋯H2O complexes

Structures and interaction energies of complexes valence isoelectronic to the important CO?H(2)O complex, namely SiO?H(2)O and CS?H(2)O, have been studied for the first time using high-level ab initio methods. Although CO, SiO, and CS are valence isoelectronic, the structures of their complexes with water differ significantly, owing partially to their widely varied dipole moments. The predicted dissociation energies D(0) are 1.8 (CO?H(2)O), 2.7 (CS?H(2)O), and 4.9 (SiO?H(2)O) kcal∕mol. The implications of these results have been examined in light of the dipole moments of the separate moieties and current concepts of hydrogen bonding. It is hoped that the present results will spark additional interest in these complexes and in the general non-covalent paradigms they represent.     

Esca study of some chromium complexes: ionization energies and multi-peak structure of the spectra

The chemical shifts of the core ionization energies of C₆H₆CrC₆H₆, C₆H₆Cr(CO)₃, COOCH₃C₆H₅Cr(CO)₃ and Cr(CO)₆ have been measured and information on the bonding of these complexes has been obtained. In the spectra of the complexes studied the main peaks have been frequently found to be accompanied by smaller ones, whose intensities and energies are structure dependent. In an attempt to assign these “extra” peaks, the energy separations from the main peak have been compared with the ultraviolet absorption energies of the neutral molecules.     

Electronic structure of H2CS3 and H2CS4: an experimental and theoretical study

The HeI photoelectron spectra of H2CS3 and H2CS4 in the gas phase have been obtained for the first time. A complete theoretical study involving the calculation of the ionization energies using orbital valence Green's functional (OVGF) and population analysis was performed. Calculations of cation-radical forms were carried out in order to interpret the main characters of the six highest occupied molecular orbitals (HOMOs). The first vertical ionization potentials are 8.74 and 8.56eV for H2CS3 and H2CS4, and attributed to {9b2(nS(C=S))}-1 and {8a"(3ppi*(S-S), nS)}-1, respectively. Meanwhile, the energy sequence of three types of sulfur 3p lone-pair have been discussed: 3ppi(S-S)*相似文献   

Density functional and Ab initio study of Cr(CO)n (n = 1-6) complexes

Cr(CO)n (n = 1-6) systems were studied for all possible spin states using density functional and high-level ab initio methods to provide a more complete theoretical understanding of the structure of species that may form during ligand dissociation of Cr(CO)6. We carried out geometry optimizations for each system and obtained vibrational frequencies, sequential bond dissociation energies (BDE), and total CO binding energies. We also compared the performance of various DFT functionals. Generally, the ground states of Cr(CO)6, Cr(CO)5, and Cr(CO)4, whose spin multiplicity is a singlet, are in good agreement with both previous theoretical results and currently available experimental data. Calculations on Cr(CO)3, Cr(CO)2, and CrCO provide new findings that the ground state of Cr(CO)3 might be a quintet with C2v symmetry instead of a singlet with C3v symmetry, and the ground state of Cr(CO)2 is not a linear quintet, as suggested by previous DFT calculations, but rather a linear septet. We also found that nonet states of Cr(CO)2 and CrCO display partial C-O bond breakage.     

Actinide sulfides in the gas phase: experimental and theoretical studies of the thermochemistry of AnS (An = Ac, Th, Pa, U, Np, Pu, Am and Cm)

The gas-phase thermochemistry of actinide monosulfides, AnS, was investigated experimentally and theoretically. Fourier transform ion cyclotron resonance mass spectrometry was employed to study the reactivity of An(+) and AnO(+) (An = Th, Pa, U, Np, Pu, Am and Cm) with CS(2) and COS, as well as the reactivity of the produced AnS(+) with oxidants (COS, CO(2), CH(2)O and NO). From these experiments, An(+)-S bond dissociation energies could be bracketed. Density functional theory studies of the energetics of neutral and monocationic AnS (An = Ac, Th, Pa, U, Np, Pu, Am and Cm) provided values for bond dissociation energies and ionization energies; the computed energetics of neutral and monocationic AnO were also obtained for comparison. The theoretical data, together with comparisons with known An(+)-O bond dissociation energies and M(+)-S and M(+)-O dissociation energies for the early transition metals, allowed for the refining of the An(+)-S bond dissociation energy ranges obtained from experiment. Examination of the reactivity of AnS(+) with dienes, coupled to comparisons with reactivities of the AnO(+) analogues, systematic considerations and the theoretical results, allowed for the estimation of the ionization energies of the AnS; the bond dissociation energies of neutral AnS were consequently derived. Estimates for the case of AcS were also made, based on correlations of the data for the other An and the electronic energetics of neutral and ionic An. The nature of the bonding in the elementary molecular actinide chalcogenides (oxides and sulfides) is discussed, based on both the experimental data and the computed electronic structures. DFT calculations of ionization energies for the actinide atoms and the diatomic sulfides and oxides are relatively reliable, but the calculation of bond dissociation energies is not uniformly satisfactory, either with DFT or CCSD(T). A key conclusion from both the experimental and theoretical results is that the 5f electrons do not substantially participate in actinide-sulfur bonding. We emphasize that actinides form strikingly strong bonds with both oxygen and sulfur.     

σ-Alane complexes of chromium, tungsten, and manganese

Photolytic ligand displacement and salt metathesis routes have been exploited to give access to κ(1) σ-alane complexes featuring Al-H bonds bound to [W(CO)(5)] and [Cp'Mn(CO)(2)] fragments, together with a related κ(2) complex of [Cr(CO)(4)]. Spectroscopic, crystallographic, and quantum chemical studies are consistent with the alane ligands acting predominantly as σ-donors, with the resulting binding energies calculated to be marginally greater than those found for related dihydrogen complexes.     

Density functional calculations of the structures and bond energies of Cr(CO)6 and (η6-C6H6) Cr(CO)2(CX) (X=O,S) complexes

Summary Quantum chemical calculations based on density functional theory have been performed on Cr(CO)₆, (⁶-C₆H₆)Cr(CO)₃ and (⁶-C₆H₆)Cr(CO)₂(CS) at the local and nonlocal level of theory using different functionals. Good agreement is obtained with experiment for both optimized geometries and metal-ligand binding energies. In particular, a comparison of metal-arene bond energies calculated for the (⁶-C₆H₆)Cr(CO)₃ and (⁶-C₆H₆)Cr(CO)₂(CS) complexes correlates well with kinetic data demonstrating that substitution of one CO group by CS leads to an important labilizing effect of this bond, which may be primarily attributed to a larger -backbonding charge transfer to the CS ligand as compared with CO.     

Comparaison des effects electroniques des ligands a deux electronx CX (X = O, S, Se) dans des complexes organometalliques du type CH3CO2(C6H5)Cr(CO)2(CX)

Structural and spectroscopic (IR, Raman) results concerning the organometallic complexes, CH₃CO₂(C₆H₅)Cr(CO)₂(CX) (X = O, S, Se) and theoretical calculations allow the comparison of electronic effects of CO, CS and CSe ligands. The strenght of the ligand---metal bond and the overall electron-with- drawing ability are higher for Se than for S and O, the largest variation being between S and O. This overall effect results in better σ-electron-repelling and π-electron-withdrawing abilities for Se than for S and O. Consequences of substituting one CO by CS or CSe in CH₃CO₂(C₆H₅)Cr(CO)₃ are analyzedin terms of molecular coordination. In particular Cr(CO)₂(CS) deformations and Cr---C (ring) bond variation are discussed. Some comparisons are made with phosphinechromium complexes.