2-十八烷基四氰代二甲基苯醌的红外光谱

采用二次微分和解卷积法，对2－十八烷基TCNQ的红外光谱数据进行处理，首次发现长碳链中CH2对称伸缩振动的分峰现象，并将CH2对称和反对称伸缩振动的分裂归结为是由十八烷基TCNQ分子中碳氢链的不同构象所产生的。     

二维红外光谱法分析聚丙烯C-H伸缩振动

在3 000~2 800cm~(-1)范围内,分别测定聚丙烯C-H伸缩振动(νC-H)的一维红外光谱、二阶导数红外光谱和四阶导数红外光谱来确定聚丙烯的分子结构。试验发现聚丙烯νC-H主要包括甲基碳氢不对称伸缩振动模式(ν_(as)CH_3)、甲基碳氢对称伸缩振动模式(ν_sCH_3)、亚甲基碳氢不对称伸缩振动模式(ν_(as)CH_2)、亚甲基碳氢对称伸缩振动模式(ν_sCH_2)和次甲基碳氢伸缩振动模式(νCH)。进一步采用二维红外光谱研究了温度对聚丙烯νC-H的影响。研究发现,随着温度的升高,聚丙烯分子中νC-H红外吸收强度变化快慢顺序为2875cm~(-1)(ν_sCH_3),2 890cm~(-1)(νCH),2 932cm~(-1)(νasCH_2),2 975cm~(-1)(νasCH_3),2 855cm~(-1)(ν_sCH_2)。     

基于亲电试剂对活泼两性离子中间体捕捉而实现的芳香碳氢键不对称官能团化

<正>Angew.Chem.Int.Ed.2014,53,13098~13101通过金属卡宾参与而实现的碳氢键官能团化是构建碳碳键的一种十分可靠和高效的方法.过去的几十年中,基于金属卡宾参与而实现的sp3碳氢键的不对称官能团化已经得到了广泛研究.然而,通过金属卡宾而实现的芳香sp2碳氢键的不对称官能团化仍面临着巨大的挑战.目前除了分子内的反应,或以较为活泼的杂原子芳香环为底物的反应被报道之外,尚无分子间的全碳芳香环sp2碳氢键的不对称官能团化被报道.华东师范大学化学系胡文浩与邢栋     

碳氟-碳氢表面活性剂混合水溶液在油面上铺展

本文研究RfCONH(CH2)3N(C2H5)2CH3I/CnH2n 1,COONa及RfCOONa/CmH2m 1N(CH3)3Br(Rf=F[CF(CF3)CF2O]2CF(CF3);n=7,8.11,13;m=8,10,12)两类正，负离子碳氟－碳氢表面活性剂混合水溶液在油面上的铺展及对油面的密封性能。研究表明在碳氟表面活性剂中加入异电性碳氢表面活性剂可大大降低碳氟表面活性剂水溶液的铺展浓度，也可使一些因素表面张力较高而不能铺展的碳氟表面活性剂水溶液在油面上铺展。在碳氟表面活性剂中加入异电性碳氢表面活性剂可提高水膜对油面的密封性。若在混合表面活性剂中加入黄原胶，水膜的密封性能更好。     

阳离子碳氢/碳氟表面活性剂与中性高聚物相互作用的研究

研究了阳离子碳氢表面活性剂十二烷基三烷基溴化铵[C12H25N(CnH2n＋1)3Br, n＝1, 2, 3, 4]和阳离子碳氟表面活性剂F[CF(CF3)CF2O]2CF(CF3)CONH(CH2)3N(C2H5)2CH3I (FCI-2)分别与中性高聚物聚氧乙烯(PEO, 分子量20000)和聚氧乙烯-聚氧丙烯三嵌段共聚物[(EO)76(PO)29(EO)76, F68]的相互作用. 结果表明, 所用的碳氢阳离子表面活性剂与PEO和F68均无相互作用, 但碳氟阳离子表面活性剂FCI-2与PEO和F68均具有明显的相互作用, 而且F68与FCI-2的相互作用强于PEO与FCI-2体系. 结果也初步表明碳氟表面活性剂与高聚物的相互作用强于碳氢表面活性剂-高聚物体系.     

傅里叶变换红外光谱对食道癌及相应正常组织的研究

研究了9例食道癌及相应正常组织的红外光谱，从光谱参数（形状、频率、强度等）方面进行了分析。结果表明：癌组织样品与政党组织样品存在明显的光谱上的差异。着重讨论了核酸中磷酸二酯基团（PO2^-)对称和反对称伸缩振动、膜脂中的碳氢基团（CH3，CH2）的伸缩及弯曲振动、蛋白质中C－O基团的伸缩振动峰的变化。从氢键角度以及膜脂碳氢链排列及构象变化角度分析了变化的原因。     

碳氟型及碳氫型乳化剂对苯乙烯及α,β,β-三氟苯乙烯乳液聚合速度的影响

用膨胀计法研究了在不同乳化剂存在下,苯乙烯及α,β,β-三氟苯乙烯的乳液聚合速 度,所用的乳化剂是:碳氟链型乳化剂H(CF_2)_nCOOK,n=6,8,10,和CF_2Cl(CFClCF_2)_3COOK及碳氢链型乳化剂H(CH_2)_nCOOK,n=8,11。在所有情况下,α,β,β-三氟苯乙烯的聚合速度都低于苯乙烯。用碳氢链羧酸盐作乳化剂时,苯乙烯与α,β,β-三氟苯乙烯的聚合速度大于用碳氟链羧酸盐作乳化剂时的聚合速度,在ω-氢全氟羧酸钾系列中,H(CF_2)_nCOOK,n=6,8,10,用n=8的羧酸钾作乳化剂时单体的聚合速度最大。     

原子个数n对碳分子线Cn(n＝3～10)基态结构特性的影响

利用密度泛函B3LYP方法, 在6-311++g**基组水平上对碳分子线Cn(n＝3～10)体系的基态电子结构特性等作了理论计算. 计算结果表明, 当n为奇数时, 碳分子线Cn基态都为单重态, 反之, 当n为偶数时, 三重态为其稳定的基态. 同时在得到碳分子线基态构型的基础上, 对其极化率、电荷分布和能级分布进行了研究, 确定了碳分子线体系最高占据轨道HOMO能量EH, 最低未占据轨道LUMO能量EL与n的关系式, 即EHn－2 < EHn < EHn+2, ELn－2 > ELn > ELn+2. 因而碳分子线Cn(n＝3～10)体系的费米能级会表现出特有的奇偶振荡, 本文也对该现象出现的原因进行了讨论.     

UF6分子的模型伸缩振动能级的计算

利用一个四参数非线性模型,对处于电子基态下的XY6型分子的X-Y键的伸缩振动进行了描述,并将其应用于计算UF6分子中U-F键的伸缩振动能级.计算中引入的模型Hamilton算符所包含的描述U-F键非谐振动的参数λ和描述U-F键之间的偶极-偶极相互作用参数ε1, ε2由实验值得出,波函数|ψn〉按形式为|n,α〉=|n1〉|n2〉|n3〉|n4〉|n5〉|n6〉的基函数集展开,从而把复杂的Hamilton方程转化为简单的矩阵代数方程.结果显示,该非线性模型能够较好地描述UF6分子的振动( 计算误差在1.0 cm-1之内 ),同时合理地预测了一些至今还未观测到的能级值.     

弱碱柔能克刚:动力学去质子官能化反应

碳氢键的去质子官能化反应是碳碳键构建最常用的方法,是一种重要的碳氢键活化方式.近年来,碱催化碳碳键形成反应在含弱酸性碳氢键化合物作为亲核试剂的底物拓展方面取得了重要进展.强碱性试剂或催化剂是实现这些弱酸性碳氢键官能化反应的关键.根据酸碱平衡理论,相对较强的碱才能够对弱酸性碳氢键发生去质子化反应,形成较大浓度的碳负离子中间体,进而发生亲核反应.相对较弱的碱不足以对弱酸性碳氢键进行去质子化反应,然而尽管碳负离子中间体可能浓度很低,但应该仍然存在于反应体系中.如果可以选择性地进行热力学有利的化学转化,碳负离子中间体的浓度将会下降并引起去质子化平衡的重新构建.结合碳负离子中间体不可逆的转化和去质子平衡的重新构建,弱酸性碳氢键就可以在弱碱条件下实现缓慢却持续不断的去质子官能化反应.为区别于强碱条件下、通过热力学稳定碳负离子中间体的传统碳氢键去质子官能化反应,我们将这种在弱碱条件下、通过热力学不利的碳负离子中间体转化和酸碱平衡重新构建实现的弱酸性碳氢键的官能化反应称为动力学去质子官能化反应.本文总结了碳氢键去质子官能化反应研究现状和本研究团队近年来在弱碱条件下的动力学去质子官能化反应研究进展.     

Structural basis for the discrepancy of spectral behavior in C-H stretching band between steroids and long chain hydrocarbon compounds

The discrepancies of the spectral behavior for the C-H stretching band between some long chain hydrocarbon compounds and steroids were investigated. At low temperature, the C-H stretching bands exhibit complex fine structure in steroids but remain simple in long chain hydrocarbon compounds. MM3 molecular mechanics calculation indicates that, for long chain hydrocarbon compounds, the C-H groups vibrate with large scale coupling. There exist a few bands where the C-H groups vibrate in synchronous and inphase mode. Thus the variations of dipole moment for these bands are enhanced and the intensities are obviously stronger than others and cover other band in the spectra. This is just the reason why the C-H stretching bands are simple even at low temperature environment. Nevertheless, for the steroids, the C-H stretching bands vibrate with local coupling mode. The synchronous enhancement effect does not occur, the differences of intensities for various modes are not as large as those in long chain hydrocarbo     

Strongly blue-shifted C-H stretches: interaction of formaldehyde with hydrogen fluoride clusters

The equilibrium structures, binding energies, and vibrational spectra of the cyclic, hydrogen-bonded complexes formed between formaldehyde, H(2)CO, and hydrogen fluoride clusters, (HF)(1< or =n < or =4), are investigated by means of large-scale second-order M?ller-Plesset calculations with extended basis sets. All studied complexes exhibit marked blue shifts of the C-H stretching frequencies, exceeding 100 cm(-1) for n = 2-4. It is shown that these blue shifts are, however, only to a minor part caused by blue-shifting hydrogen bonding via C-H...F contacts. The major part arises due to the structural relaxation of the H(2)CO molecule under the formation of a strong C=O...H-F hydrogen bond which strengthens as n increases. The close correlation between the different structural parameters in the studied series of complexes is demonstrated, and the consequences for the frequency shifts in the complexes are pointed out, corroborating thus the suggestion of the primary role of the C=O...H-F hydrogen bonding for the C-H stretching frequency shifts. This particular behavior, that the appearance of an increasingly stronger blue shift of the C-H stretching frequencies is mainly induced by the formation of a progressively stronger C=O...H-F hydrogen bond in the series of H(2)CO...(HF)(1< or =n < or =4), complexes and only to a lesser degree by the formation of the so-called blue-shifting C-H...F hydrogen bond, is rationalized with the aid of selected sections of the intramolecular H(2)CO potential energy surface and by performing a variety of structural optimizations of the H(2)CO molecule embedded in external, differently oriented dipole electric fields, and also by invoking a simple analytical force-field model.     

Infrared spectroscopic ellipsometry of n-alkylthiol (C5-C18) self-assembled monolayers on gold

The infrared spectroscopic ellipsometry (IRSE) of n-alkylthiol (CH3(CH2)xSH, x = 4, 6, 7, 8, 10, 13, 15, and 17, self-assembled monolayers (SAMs), with 5-18 carbon atoms (C5-C18), grown on gold-coated Si(100) substrates) was investigated at room temperature. The C-H stretching vibrations could be resolved even for pentathiol, the shortest chain studied. The symmetric and asymmetric stretching vibrations of the CH2 groups are located at about 2850 and 2920 cm(-1), and those of CH3 are at about 2877 and 2962 cm(-1), respectively; they show a slight shift with the number of CH2 units. In addition, Fermi resonance of the symmetric CH3 stretching vibration at 2940 cm(-1) appears with decreasing chain length due to weak coupling with the asymmetric CH2 stretching vibration. The "odd-even effect" of the n-alkylthiol SAMs with varying CH2 units could be distinguished by the two interactive IRSE parameters. The relative ellipsometric spectra for the four longest chains could be reproduced quite well by using a Lorentz multioscillator model with a three-phase optical model (air/SAMs/gold). On the basis of the theoretical calculations, the vibrational strength of these oscillators is very weak, its magnitude being 10(-4)-10(-5). The full width at half-maximum (fwhm) of the peaks varies from 7 to 33 cm(-1). Moreover, the intensity of the C-H vibrations increases with the number of methylene units, due to strong lateral interactions and ordering effects occurring for longer chains.     

Coordination structures of lithium-methylamine clusters from infrared spectroscopy and ab initio calculations

Spectra of clusters formed between lithium atoms and methylamine molecules are reported for the first time. Mass-selective infrared spectra of Li(NH(2)CH(3))(n) have been recorded in both the N-H and C-H stretching fundamental regions. The infrared spectra are broadly in agreement with ab initio predictions, showing redshifted N-H stretching bands relative to free methylamine and a strong enhancement of the N-H stretching fundamentals relative to the C-H stretching fundamentals. The ab initio calculations suggest that, for n=3, the methylamine molecules bunch together on one side of the lithium atom to minimize repulsive interactions with the unpaired electron density. The addition of a fourth methylamine molecule results in closure of the inner solvation shell and, thus, Li(NH(2)CH(3))(5) is forced to adopt a two-shell coordination structure. This is consistent with neutron diffraction studies of concentrated lithium/methylamine solutions, which also suggest that the first solvation shell around the lithium atom can contain a maximum of four methylamine molecules.     

IR spectroscopic investigation of cis-(CH(3))(2)Au(O,O'-acac) and cis-(CD(3))(2)Au(O,O'-acac)

The IR spectrum of cis-(CH(3))(2)Au(O,O'-acac) has been reassigned by comparing frequencies for cis-(CH(3))(2)Au(O,O'-acac) and cis-(CD(3))(2)Au(O,O'-acac), and by analysis of the DFT-calculated normal modes and their frequencies for the isolated molecules. The vibrational intensity in the C-H stretching region arises almost entirely from the cis-(CH(3))(2)Au fragment, while the methyl deformation intensity is largely of acetylacetonato ligand origin. A low frequency mode in the C-H stretching region is the first overtone of the delta(a)(CH(3)) mode of cis-(CH(3))(2)Au. The Au-C stretching modes are affected by deuteration of the cis-(CH(3))(2)Au fragment, while the Au-O stretching modes are not.     

An ab initio calculation of the dissociation C2H2(1Σ+) → C2H(2Σ+) + H(2S)

The collinear dissociation of acetylene to C₂H and H is studied by a generalized self-consistent procedure. The dissociation energy, the C-H force constant and stretching frequency are computed.     

系列化合物C-H伸缩频率的自然杂化轨道研究

在计算C-H核自旋-自旋偶合常数的新公式及其与C-H伸缩频率之间的关系的基础上, 得出了计算C-H伸缩频率的新的一般关系式。并利用CNDO/2分子轨道和自然杂化轨道方法, 具体计算了三种不同系列化合物的原子净电荷和自然杂化轨道。给出了计算不同系列化合物C-H伸缩频率的良好线性关系式。结果表明, 碳氢化合物中的C-H伸缩频率主要由原子的轨道杂化作用所决定, 而对于含杂原子的取代碳氢化合物, C-H键的极性成为影响伸缩频率的重要因素。     

Experimental evidence for intramolecular blue-shifting C-H...O hydrogen bonding by matrix-isolation infrared spectroscopy

Experimental evidence for intramolecular blue-shifting C-H...O hydrogen bonding is presented. Argon matrix-isolation infrared spectra of 1-methoxy-2-(dimethylamino)ethane exhibit a band at 3016.5 cm-1. Spectral behavior with annealing indicates that this band is assigned to the most stable conformer, trans-gauche-(trans|gauche'), with an intramolecular C-H...O hydrogen bond. Density functional calculations show that this band arises from the stretching vibration of the C-H bond participating in the formation of the C-H...O hydrogen bond. The C-H bond is shortened by 0.004 A, and the C-H stretching band is blue-shifted by at least 35 cm-1 on the formation of the hydrogen bond. The (C)H...O distance is calculated as 2.38 A, which is shorter than the corresponding van der Waals separation by 0.3 A.     

Adsorption of 1- and 2-butylimidazoles at the copper/air and steel/air interfaces studied by sum frequency generation vibrational spectroscopy

The structure of thin films of 1- and 2-butylimidazoles adsorbed on copper and steel surfaces under air was examined using sum frequency generation (SFG) vibrational spectroscopy in the ppp and ssp polarizations. Additionally, the SFG spectra of both isomers were recorded at 55 °C at the liquid imidazole/air interface for reference. Complementary bulk infrared, reflection-absorption infrared spectroscopy (RAIRS), and Raman spectra of both imidazoles were recorded for assignment purposes. The SFG spectra in the C-H stretching region at the liquid/air interface are dominated by resonances from the methyl end group of the butyl side chain of the imidazoles, indicating that they are aligned parallel or closely parallel to the surface normal. These are also the most prominent features in the SFG spectra on copper and steel. In addition, both the ppp and ssp spectra on copper show resonances from the C-H stretching modes of the imidazole ring for both isomers. The ring C-H resonances are completely absent from the spectra on steel and at the liquid/air interface. The relative intensities of the SFG spectra can be interpreted as showing that, on copper, under air, both butylimidazoles are adsorbed with their butyl side chains perpendicular to the interface and with the ring significantly inclined away from the surface plane and toward the surface normal. The SFG spectra of both imidazoles on steel indicate an orientation where the imidazole rings are parallel or nearly parallel to the surface. The weak C-H resonances from the ring at the liquid/air interface suggest that the tilt angle of the ring from the surface normal at this interface is significantly greater than it is on copper.     

Blue-shifted A-H stretching modes and cooperative hydrogen bonding. 1. Complexes of substituted formaldehyde with cyclic hydrogen fluoride and water clusters

The structures and vibrational spectra of the intermolecular complexes formed by insertion of substituted formaldehyde molecules HRCO (R = H, Li, F, Cl) into cyclic hydrogen fluoride and water clusters are studied at the MP2/aug-cc-pVTZ computational level. Depending on the nature of the substituent R, the cluster type, and its size, the C-H stretching modes of HRCO undergo large blue and partly red shifts, whereas all the F-H and O-H stretching modes of the conventional hydrogen bonds are strongly red-shifted. It is shown that (i) the mechanism of blue shifting can be explained within the concept of the negative intramolecular coupling between C-H and C=O bonds that is inherent to the HRCO monomers, (ii) the blue shifts also occur even if no hydrogen bond is formed, and (iii) variation of the acceptor X or the strength of the C-H...X hydrogen bond may either amplify the blue shift or cause a transition from blue shift to red shift. These findings are illustrated by means of intra- and intermolecular scans of the potential energy surfaces. The performance of the negative intramolecular coupling between C-H and C=O bonds of H(2)CO is interpreted in terms of the NBO analysis of the isolated H(2)CO molecule and H(2)CO interacting with (H2O)n and (HF)n clusters.