质子化丙酮分子团簇的结构和振动光谱

The stable structures and vibrational spectra of protonated acetone molecule clusters with different sizes （CH3COCH3）nH +（n=1-7）are calculated at the 6-31G（d）level by means of density functional theory （B3LYP）quantum chemical calculations. The corresponding energies are analyzed at the level B3LYP/6-311+G（3df,2p）in order to obtain more accurate results. The proton affinity of neutral cyclic acetone molecule clusters increases with the increasing of cluster size. The calculated results show that the protonated acetone clusters have certain growth regularity with forming a solvation shell at the beginning and then new added acetone molecule attacking different active sites including the middle carbon atoms and the different methyl in solvation shell. The IR spectra of the protonated clusters are more complicate than that of neutral ones. The strongest peaks result from the movement of the proton between the two oxygen atoms in solvant shell apart from the case of n=1. Carbonyl stretching vibraional peaks split into the more and more and in general the corresponding intensities are weakened due to the protonation with the increasing of cluster size.     

铂配位的腺嘌呤质子化的理论研究

用量子化学从头算研究一系列平面四方金属配体作用于腺嘌呤N₇位点对其质子化的影响。计算结果表明气相中，配合物质子化能力主要受长程静电效应影响，不同金属离子的影响差别甚微。综合考虑极性溶剂影响后长程静电效应影响显著降低。NBO电荷布居分析表明质子化位点电子云密度的变化直接影响该位点质子化能力。     

马钱子碱分子结构和振动光谱的密度泛函理论研究

用密度泛函理论B3LYP/6-31G*方法对天然药材马钱子中的生物碱马钱子碱的几何构型进行了优化,得到马钱子碱分子的平衡结构参数,并同实验结构进行了比较.计算了上述分子在平衡构型下的振动谐力场和振动基频.针对不同的振动模式,提出了相应的校正因子,并据此对计算频率进行了校正.理论计算和实验测定频率的平均误差为19.0cm-1.根据DFT计算的振动模式和IR光谱强度值对目标分子的实验振动基频进行了完善的和合理的指认和解释.     

Ti-MWW分子筛正弦孔道内骨架钛物种的结构和红外振动光谱的理论计算

应用密度泛函理论计算,研究了Ti-MWW分子筛10元环正弦孔道内骨架钛物种的结构和振动光谱。计算采用基于36T簇模型的B3LYP/6-31G(d,p)方法,确定了[Ti(OSi)₄]物种优先落位于T3位,在924~987cm^-1区域内存在3个振动峰,都属于以Ti为正四面体中心分布的4个Ti-O-Si键的协同伸缩振动,其中958cm^-1的振动强度较大,属于[Ti(OSi)₄]的特征频率。T2和T8位上钛物种不出现该特征峰。Ti(Ⅳ)中心上吸附一个水分子形成五配位配合物,其特征振动频率没有变化。[Ti(OSi)₄]物种进一步水解形成[Ti(OSi)₃OH]物种,其Ti-O-Si的特征振动蓝移到969cm^-1。此外,还考察了Ti-MWW分子筛中可能存在的骨架硼以及羟基巢的结构和振动光谱,计算频率与已有文献数据相符。     

质子化和脱质子化对酞菁光谱的影响

系统地研究四异丙氧基酞菁的子化和脱质子化对吸收和发射光谱的影响，研究表明，三氟乙酸可对酞菁分子连续质子化，分别生成（Ｈ２Ｐｃ（Ｏ＾ｉＰｒ）４．Ｈ＾＋）＾和（Ｈ２Ｐｃ（Ｏ＾ｉＰｒ）４．２Ｈ＾＋）＾２＋，而硫酸可使酞菁形成（Ｈ２Ｐｃ（Ｏ＾ｉＰｒ）４．４Ｈ＾＋＾４＋此外，ＮａＯＨ／ＥｔＯＨ可使酞菁分子脱质子化生成（Ｐｃ（Ｏ＾ｉＰｒ）４）＾２－反应一步完成，表明分子中的两个吡咯－ＮＨ－同步酸解，质子化可使     

Ti-MWW分子筛吸附H2O和NH3的结构和振动光谱的密度泛函理论计算

Ti-MWW分子筛具有10元环(10MR)孔道体系和12MR超笼以及外表面杯状空穴,在以H2O2水溶液为氧化剂的催化氧化反应中表现出不同于其他钛硅分子筛的特殊溶剂效应和立体选择性.已有的实验和密度泛函理论(DFT)计算研究表明,骨架Ti(IV)可能分布在10MR孔道和12MR超笼中.最近,我们采用DFT计算研究了Ti-MWW分子筛中骨架钛落位,通过比较Ti/Si替代能和红外振动光谱,提出Ti(IV)最可能落位在T1和T3位,并以[Ti(OSi)4]形态存在,显示960 cm–1钛特征振动峰.[Ti(OSi)4]物种水解时Ti–O键发生选择性断裂,生成具有翻转Ti–OH的[Ti(OSi)3OH]物种.由于Ti中心具有Lewis酸性,与配体分子络合后使Ti(IV)的配位状态改变. Ti-MWW分子筛中不同的骨架Ti(IV)落位和形态可能呈现不同的催化选择性.本文应用DFT研究了Ti-MWW分子筛中T1和T3位上不同钛物种与H2O和NH3的吸附作用,考察了其几何结构、吸附能以及红外振动光谱性质,为深入理解骨架Ti(IV)的微观结构及实验红外光谱表征提供参考数据.计算采用36T簇模型,从MWW分子筛晶体结构中分别以T1和T3为中心截取七层骨架原子,末端设为Si–H键并固定为1.46?.结构优化时松弛内部四层骨架原子并固定最外三层骨架原子.所有计算在B3LYP/6-31G(d,p)理论水平完成,计算的吸附能都经过BSSE校正,计算的频率以约化因子0.961校正.所有计算在Gaussian 09软件包完成.计算结果表明,四配位的[Ti(OSi)4]和[Ti(OSi)3OH]物种都能与H2O或NH3分子作用生成三角双锥的五配位络合物. H2O或NH3分子有选择性地进攻Ti–O键的Ti端,形成近乎直线的L–Ti–O键, L–Ti距离可达2.2–2.4?. T1位钛物种的Lewis酸性比T3位的略高.对于[Ti(OSi)3OH]物种, Ti–OH的存在使得Ti(IV)的酸性大大增强,表现出很强的吸附作用.此外,[Ti(OSi)3OH]物种也能通过Ti–OH基团与H2O和NH3形成氢键络合物,但是其吸附能比形成配位络合物的能量更小,说明配体分子更趋向于吸附在Ti中心形成配位络合物.自然键轨道分析表明, Ti(IV)中心的Lewis酸性归因于Ti的空4p轨道接受配体提供的孤对电子,并且属于LUMO+3.所有吸附络合物的特征振动频率分布在两个区域,即钛特征振动区域和羟基振动区域. T1和T3位的[Ti(OSi)4]物种的钛特征振动频率都在960 cm–1,与H2O形成五配位的吸附络合物之后,钛特征振动频率位移到970 cm–1.[Ti(OSi)3OH]物种的钛特征振动频率分别为990 cm–1(T1位)和970 cm–1(T3位),吸附H2O分子后都位移到980 cm–1.相应的NH3吸附络合物的钛特征振动峰频率都高出5 cm–1.分析表明,钛特征振动模式归属于Ti–O–Si键的不对称伸缩振动的协同振动.在羟基伸缩振动区域,气相H2O、末端Si–OH基团以及Ti–OH基团的羟基伸缩振动在3600–3760 cm–1.吸附H2O后,羟基伸缩振动移到3460–3150 cm–1区域.[Ti(OSi)3OH]物种与NH3和H2O形成氢键络合物后,钛羟基的伸缩振动频率分别红移500和1100 cm–1,出现在2700和3200 cm–1区域.吸附分子的O–H和N–H的伸缩振动频率略微蓝移,这反映了Ti物种具有Lewis酸性.     

去氢抗坏血酸分子振动光谱的理论研究

采用RHF, MP2, DFT(B3LYP)方法, 以6-311++G**为基组研究了去氢抗坏血酸分子(DHA)的平衡几何构型和振动光谱. 计算结果表明, 采用RHF, B3LYP以及MP2 方法优化得到的几何结构以及频率值是一致的. 采用B3LYP/6-311++G**计算了DHA分子平衡构型下的谐振动力场﹑振动频率和振动强度. 使用Wilson的GF矩阵方法对DHA分子进行了简正坐标分析, 依据所得的势能分布对DHA分子的振动基频进行了合理的理论归属.     

磷酸可待因的振动光谱研究

运用密度泛函理论(DFT)计算了磷酸可待因的拉曼和红外光谱.采用B3LYP混合泛函和6-31G基函数组,同时在实验上测量了磷酸可待因的常规拉曼光谱(NRS)和红外吸收光谱(IRS),结果表明:在振动频率上理论结果与实验结果相当一致,根据理论计算的结果对磷酸可待因的振动光谱进行分析,通过理论与实验数据的比较,对磷酸可待因的所有振动谱带进行了全面地归属.     

间二甲氧基苯的分子结构、振动光谱和电离能

运用从头算和密度泛函理论方法，找到间二甲氧基苯有三种异构体，分析了它们在电子基态、第一电子激发态和离子态的分子结构；采用单色共振双光子电离方法，得到了间二甲氧基苯的单色共振双光子电离光谱；运用双色共振双光子电离的方法，测定了间二甲氧基苯三种异构体的电离能。结果表明：间二甲氧基苯的三种异构体中，异构体a最稳定；间二甲氧基苯的单色共振双光子电离光谱中的很多振动与环平面内的振动模式有关；间二甲氧基苯三种异构体的电离能分别为63521、64487和63755 cm^-1。     

儿茶素结构和振动光谱的密度泛函理论研究

本文利用密度泛函理论方法B3LYP在6-311 G(d,p)水平上研究了儿茶素及其异构体表儿茶素分子的几何构型,计算结果与实验所得结构参数一致.计算了儿茶素分子平衡构型下的力常数,使用Wilson的GF矩阵方法计算了振动基频以及相应的势能分布,据此结合理论计算的光谱强度,对儿茶素分子的振动基频进行了完善合理的理论归属.     

丙酮酸分子结构与振动光谱的密度泛函理论研究

用密度泛函方法BLYP、B3LYP和从头算Hartree-Fock(HF)方法在6-31G*基组水平上对丙酮酸分子的几何结构（甲基的重叠式和交错式两种构象）和振动光谱分别进行了优化和计算,并给出了各种频率所对应的红外强度及拉曼活性,对光谱进行了指认。结果表明：在丙酮酸分子的两种构象中,重叠式比较稳定*B3LYP计算得到的构型参数与实验结果比较一致;在振动频率的计算中,BLYP未标度力场所计算的非CH3伸缩振动基频预测值和实验值的平均绝对偏差为10.4cm-1;而HF标度力场的平均绝对偏差为17.9cm-1。说明两者的结果与实验观测频率比较吻合,但B3LYP的频率计算值偏差（38.3cm-1）较大。根据振动频率的势能分布和红外光谱强度对此分子的振动基频进行了理论归属。     

尿素分子振动光谱的密度泛函理论研究

用密度泛函理论方法BLYP/6-31¹⁺+G(2df,2pd)对尿素分子的平衡几何构型进行了优化,并计算了该分子的谐力场.使用Wilson的GF矩阵方法,对尿素分子的振动基频进行了理论研究.根据振动频率的势能分布对此分子的振动基频进行了理论归属,计算的振动频率和能级指认均同实验结果吻合较好.     

Vibrational Spectra and Density Functional Theory Calculations of Metallotriphenylcorroles

The infrared absorption and Raman scattering spectra were measured for the metallotriph-enylcorroles (MTPCs, M=Cu, Co, Ni, Mn). The ground-state structures and vibrational spectra of MTPCs have been calculated with the density functional theory. The observedRaman and IR bands have been assigned based on the calculation results. Due to the symmetry lowering, the vibrational spectra of MTPCs are much more complex than metal-loporphyrins, and several skeletal modes are found strongly coupled to the phenyl vibrations.The relationship between the Raman/IR frequencies and the structures of TPC ring is in-vestigated. It is found that the vibrations involving the C^I_αC^I_α stretch and C_αC_mstretch are sensitive to the size of corrole core. In particular, the frequency of υ₅, which is assigned to C^I_αC^I_α stretch in coupling with the C_αC_m symmetric stretch, increases linearly with the decrease of the corrole core-sizes and may be used as a mark band to evaluate the structural change of the metallocorroles.     

二苯基乙二酮结构和电子光谱的理论研究

基于二苯基乙二酮结构优化,在TD-B3LYP/6-31+G*水平上讨论了两个异构体在气相和液相中的吸收和发射光谱.溶液中的计算采用可极化连续介质模型.结果表明,溶剂极性增加更有利于顺式非平面构型的形成,两个异构体的T1和S1态以及顺式非平面结构的S2态都源于双羰基上的n→π*.     

Vibrational Spectra and Density Functional Theory Calculations of Metallo-tetra-(tert-butyl)-tetra-azaporphyrines

The infrared absorption and 514.5 nm excited Raman spectra were measured for the metallo-tetra-(tert-butyl)-tetraazaporphyrin (MT(tBu)TAP, M=Cu, Co, Ni, Zn). The ground-state structures and vibrational spectra of MT(tBu)TAPs have been calculated at the B3LYP level of theory. The observed Raman and IR bands have been assigned based on the calculation results and by comparing with the normal metalloporphyrins. The relationship between the Raman/IR frequencies and the structures of TAP ring was investigated. The results show that the frequencies of C_βC_β′ stretch (A_g), asymmetric C_αN_m stretch (A_g), and symmetric C_αN_m stretch (B_g) modes increase linearly with the decrease of the core-sizes of TAP ring.Among the three modes, the later two are more sensitive to the core-size change.     

Vibrational Spectra and Quantum Calculations of Ethylbenzene

Normal vibrations of ethylbenzene in the first excited state have been studied using resonant two-photon ionization spectroscopy. The band origin of ethylbenzene of S₁←S₀ transition appeared at 37586 cm^-1. A vibrational spectrum of 2000 cm^-1 above the band origin in the first excited state has been obtained. Several chain torsions and normal vibrations are obtained in the spectrum. The energies of the first excited state are calculated by the time-dependent density function theory and configuration interaction singles (CIS) methods with various basis sets. The optimized structures and vibrational frequencies of the S₀ and S₁ states are calculated using Hartree-Fock and CIS methods with 6-311++G(2d,2p) basis set. The calculated geometric structures in the S₀ and S₁ states are gauche conformations that the symmetric plane of ethyl group is perpendicular to the ring plane. All the observed spectral bands have been successfully assigned with the help of our calculations.     

Density Functional Theory Investigation of Structures and Electronic Spectra of N-protonated Corroles

The geometries and electronic spectra of a series of N-protonated corroles, including unsub-stituted H₄Cor⁺ and meso-triaryl substituted H₄TPC⁺, H₄TpFPC⁺, and H₄TdCPC⁺, were theoretically studied with density functional theory (DFT). The results indicate that all these compounds have two conformers, one with C₂ symmetry (denoted as S1) is more stable than the other (denoted as S2, C₁ symmetry) by 15.8?18.5 kJ/mol. The corrole macrocycles of these compounds show significant out-of-plane deformation. The enantiomerizations of the chiral S1 conformers were found to be a multi-step process with the S2 conformers as the in-termediates. Electronic absorption spectra and electronic circular dichroism (ECD) of these compounds were calculated with time-dependent DFT. In comparison with H₄Cor⁺, the UV-Vis absorptions of meso-triaryl species are significantly red-shifted and their Q bands are enhanced due to the π-π conjugation between the aryl and corrole rings. Several neighboring electronic transitions were calculated with opposite signs in rotatory strengths, suggesting that ECD spectroscopy may be a useful tool in studying the electronic transitions of these compounds.     

Theory Study on Structures and Vibrational Frequencies of Pyruvic acid

Anumberoftheoreticalstudiesexistforpyruvicacid.IthasbeenstudiedatthesemiempiricalINDOandAMIlevell'2.AttheahinitiolevelstudiesofpyruvicacidrangefromthecalculationofenergiesattheSTO-3Glevel'tocalculationsofenergiesusingtheHF/3-2iG',HF/4-21G',HF/6-3iG*andMP2/4-21Gmethods.ExceptforthestudyofMurtoetal.,allthestudieshavefocussedontheenergiesandgeometriesofpyruvicacid.Moreoveralltheexistingtheoreticalstudieshavefocusedtheirattentionontheorientationofthecarboxylhydrogenextensively.Theorienta…