3—（9—芴甲氧基羰基）—四氢噻唑—2—硫酮振动光谱的简正坐标分析

本文采用简化一般价力场对３－（９－芴甲氧基羰基）－四氢噻唑－２－硫酮（简称Ｆｍｏｃ－ＴＴＴ）分子的振动光谱做了简正坐标分析计算，得到了一套合理的精化力常数。并对Ｔｍｏｃ－ＴＴＴ分子的振动频率进行了指认。其计算频率与实验频率的平均百分误差为０．６９１。     

异丙醇的O-H伸缩振动泛频光谱和分子构像

使用高灵敏的光腔衰范光谱（Ｃａｕｉｔｙ Ｒｉｎｇ Ｄｏｗｎ Ｓｐｅｃｔｒｏｓｃｏｐｙ）技术测出了异丙醇的Ｏ－Ｈ伸缩ｖ＝４、５振动泛频光谱,每个技动能级都有三个吸收峰,被归属为分子构像的Ｏ－Ｈ伸缩泛叔汲收,给出了光腔衰范光谱的振动泛频吸收的振动谱强度公式,并求得分子不同构在不同振动能级的Ｏ－Ｈ伸缩局域模振子的机械频率（Ｘ１）、非谐性（Ｘ２）以及解离能（Ｄ）,用浓度泛函（ＤＦＴ）Ｂ３ＬＹＰ／６－３１＋     

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Ｃ     

核介质中核子－核子散射截面的BHF微观计算

在Ｂｒｕｅｃｋｎｅｒ－Ｈａｒｔｒｅｅ－Ｆｏｃｋ（ＢＨＦ）框架下，计算了核介质中核子－核子（Ｎ－Ｎ）散射总截面．计算中，Ｎ－Ｎ相互作用势采用Ｐａｒｉｓ势的可分离表示，单粒子谱采用连续选择．计算结果表明，质子－质子散射及质子－中子散射的总截面随核密度的增加而强烈地减小，特别是对低能散射．对结果作了简单的讨论，并与已有的一些计算结果进行了比较．     

2,4—二氨基—1,3—环丁烷二酮分子的二阶超极化率和电子相关效应

在６－３１Ｇ＊＊水平上优化了２,４－二氨基－１,３－环丁烷二酮（ＮＤＱ）的分子构型,并计算了振动频率。分别用有限场方法（ＦＦ）及耦合微扰方法（ＣＰＨＦ）在ａｂ ｉｎｉｔｉｏ／４－３１Ｇ＋ｐｂ／ｐ水平上计算值较ＲＨＦ增大９％和７８％。用三态模型对计算结果进行了分析。     

BS分子α带系A~2Π→X~2Σ~+及γ带系C~2Π→X~2Σ~+法兰克-康登因子的计算

在双原子分子核运动的薛定谔方程中，计入分子的振转相互作用项，在Ｍｏｒｓｅ势近似下得出的波函数除与振动量子数有关外，还与转动量子数有关。本文用该波函数编程计算了ＢＳ分子α带系Ａ２Π→Ｘ２Σ＋及γ带系Ｃ２Π→Ｘ２Σ＋法兰克－康登（Ｆｒａｎｃｋ－Ｃｏｎｄｏｎ）因子（简称Ｆ－Ｃ因子）。计算中转动量子数的取值由Ｊ＝０至Ｊ＝２００，其结果适用于低温、高温和强激波条件。     

钬的三噻吩甲酰二氟丙酮二水配合物的简正振动分析研究

在两个简化结构模型的基础上，应用ＮＯＲＶＩＢ程序对Ｈｏ（ＴＴＡ）３２Ｈ２Ｏ分子在１６５０～１００ｃｍ－１波数范围的振动频率作了指认。在简正频率的计算值与实验值拟合优化后，确定了伸缩、弯曲、面外摇动和扭动等２１个力常数以及９个相互作用力常数。计算值与实验值之间的平均偏差为４．７５ｃｍ－１。     

PH^0—1＋1—3离解能和电离能的精确ab initio计算

对ＰＨｎ，ＰＨ＾＋ｎ（ｎ＝１～３）及其一些构型反转过渡态的几何构型用ＭＰ２（ｆｕｌｌ）／６－３１Ｇ（ｄ，ｐ）解析梯度方法优化，同时在该级别上计算了分子振动频率和零点振动能，在此基础上，分别采用Ｇａｕｓｓｉａｎ－９４程序中最大的预置基组６－３１１＋＋Ｇ（３ｄｆ，３ｐｄ）和Ｄｕｎｎｉｎｇ基组ａｕｇ－ｃｃ－ｐＶＴＺ，在冻结苡电子相关能（ＦＣ）与非冻芯模型（ｆｕｌｌ）情况下，用高级别量比化学ａｂｉｎｉｔｏ     

乙烯基吡咯烷酮－醋酸乙烯酯共聚物对1－苯胺基萘－8－磺酸盐水溶液的荧光特性的影响

将荧光探针１－苯胺基萘－８－磺酸盐（ＡＮＳ）加入到乙烯基吡咯烷酮（ＶＰ）－醋酸乙烯酯（ＶＡＣ）共聚物溶液中，共聚物组成分别为ＦＶＰ＝０．８４；０．７４；０．７０；０．５５（以乙烯基吡咯烷酮结构单元的分子数表示）。实验结果表明：ＶＰ－ＶＡＣ共聚物对ＡＮＳ水溶液的荧光强度增强效应与共聚物中乙烯基毗咯烷酮在链节中的比例有关，其组成为ＦＶＰ＝０．５５的共聚物对ＡＮＳ水溶液有显著的荧光增强效应，相对荧光强度比ＰＶＰ均聚物大一倍，而其他组成的共聚物／ＡＮＳ溶液的相对荧光强度只与溶液中ＶＰ结构单元的含量有关。这种现象说明接近等分子比的乙烯基吡咯烷酮－醋酸乙烯酯共聚物与ＡＮＳ分子间形成的过渡态结构有利于能量转移，能产生较高的量子收率，可作为电子转移反应能量转移介质。在生化反应中，可模拟酶反应机理，因而有一定的理论意义和实际意义。     

Fermi—Dirac关联与Q~（－v）K_v（Q）分布

根据非微扰理论提出一种源分布─—Ｑ－ｖＫｖ（Ｑ）分布．由此计算两质子的Ｆｅｒｍｉ－Ｄｉｒａｃ关联．拟合的曲线与实验数据吻合得较好，这是Ｑ－ｖＫｖ（Ｑ）分布比Ｇａｕｓｓ源分布优越之处．由全同质子的Ｆ—Ｄ关联计算出发射源半径及Ｆｅｒｍｉ场的反常量纲．     

芳胺基硫脲类化合物的红外光谱研究

利用烃基异硫氰酸酯分别与邻肼基苯甲酸，５－溴邻肼基苯甲酸，３，５－二溴邻肼基苯甲酸的加成反应，合成了１１种未见文献报道的芳胺基硫脲烃化合物，通过对这些化合物的红外光谱的分析和比较，归属了它们的主要红外吸收峰，考察了主要吸收峰随取代基变化规律。     

互叶白千层不同部位油细胞分布及显微拉曼光谱研究

为避免复杂的制样提取过程,在天然状态下获得植物样品油细胞中精油的成分,用显微拉曼光谱仪,得到互叶白千层同一植株不同部位的油细胞的分布及油细胞中的主成分。对各部位的显微镜观察发现在软枝干中不存在油细胞或者很少,老叶中的油细胞没有新叶中的多。在老叶油细胞上获得的谱峰中,1 675和726 cm-1为4-萜烯醇的特征峰, 归属为C═C伸缩振动和环的变形振动;1 700和754 cm-1为γ-松油烯的特征峰,归属为C═C伸缩振动和环的变形振动;1 609 cm-1为α-松油烯的特征峰,归属为C═C伸缩振动;1 522,1 156和1 011 cm-1为β-胡萝卜素的的特征峰,分别归属为C═C伸缩振动、C-C伸缩振动和C-C面内摇摆振动。在新叶油细胞上获得的谱峰中,745 cm-1为顺香桧烯水合物的特征峰,归属为环变形振动;1 609 cm-1为α-松油烯的特征峰;1 525,1 160和1 008 cm-1为β-胡萝卜素的的特征峰;老叶与新叶油细胞中的主成分不完全相同,老叶中油细胞精油为γ-松油烯-4-萜烯醇-α-松油烯型,而新叶中油细胞中的精油为顺香桧烯水合物-α-松油烯型。老叶、新叶的共有物为：α-松油烯、β-胡萝卜素。β-胡萝卜素及顺香桧烯水合物为首次在互叶白千层中发现。利用该方法可迅速的确定植株油细胞的主成分,为互叶白千层精油提取提供有益参考。     

Effect of ultrasound on the characteristics of superplastic deformation

The deformation of aluminum–lithium alloy 1420 is investigated in the region of temperatures of its superplasticity T = 320–395°C under the simultaneous action of stretching load and axial ultrasonic vibrations. The estimates of the activation parameters of deformation show that the activation energy of deformation during stretching with ultrasonic vibrations and without them are close both at the stage of hardening and at the stage of softening. It is concluded that the ultrasonic vibrations facilitate intragranular deformation at the hardening stage and promote an increase in its contribution to the total deformation without changing the deformation mechanisms.     

Vibrational Spectroscopic and Theoretical Studies of Urea Derivatives with Biochemical Interest: N,N′-Dimethylurea,N,N,N′,N′-Tetramethylurea,and N,N′-Dimethylpropyleneurea

Abstract

Mid-infrared, far-infrared, and Raman vibrational spectroscopic studies were combined with density functional theory (DFT) calculations and normal coordinate force field analyses for N,N′-dimethylurea (DMU), N,N,N′,N′-tetramethylurea (TMU), and N,N′-dimethylpropyleneurea (DMPU: IUPAC name 1,3-dimethyltetrahydropyrimidin-2(1H)-one). The equilibrium molecular geometry of DMU (all three conformers), TMU, and DMPU and the frequencies, intensities, and depolarization ratios of their fundamental infrared (IR) and Raman vibrational transitions were obtained by DFT calculations. The vibrational spectra were fully analyzed by normal coordinate methods as well. A starting force field for DMPU was obtained by adapting corresponding force constants for DMU and TMU, resulting after refinements in the stretching force constants C=O (7.69, 7.30, 7.68 N·cm^?1), C–N (5.16, 5.55, 5.05 N·cm^?1), and C-Me (5.93, 4.00, 4.22 N·cm^?1) for DMU, TMU, and DMPU, respectively. The dominating conformer of liquid DMU was identified as trans-trans, strong intermolecular hydrogen bonding was verified in solid DMU, and weak dipole–dipole association was found in liquid TMU and in DMPU. Special attention was paid to analyzing the methyl group frequencies, which revealed deviations from local C_3v symmetry. A linear correlation was found between the CH stretching force constants and the inverse of the CH bond lengths (1/r ²). The averaged NH stretching frequencies of gaseous, dissolved, and solid urea and of DMU, with variations for hydrogen bonding of different strength, are linearly correlated to the NH stretching force constants. Characteristic skeletal vibrations were assigned for a broad variety of urea derivatives and also for pyrimidine derivatives, which all contain the N₂C=O entity. The very strong IR bands of C=O stretching (1,676 ± 40 cm^?1) and asymmetric CN₂ stretching (1,478 ± 60 cm^?1), and the very intense Raman feature of symmetric CN₂ stretching or ring breathing (757 ± 80 cm^?1), can be recognized as fingerprint bands also for the pyrimidine derivatives cytosine, thymine, and uracil, which all are nucleobases in DNA and RNA nucleotides.     

Concentration‐dependent frequency shifts of the CS stretching modes in ethylene trithiocarbonate studied by Raman spectroscopy

Resonant with the CS π → π* electronic transition, the intensity of CS stretching and its overtone have been greatly enhanced in the 488‐ and 319‐nm excited resonance Raman spectra. The isotropic and anisotropic parts of the Raman spectra of CS stretching modes of ethylene trithiocarbonate (ET) at different concentrations have been analyzed in order to study the noncoincidence effect (NCE). In neat ET, the experimentally measured values of noncoincidence Δυ_nc are ~4.60 cm⁻¹ for the CS stretching modes, which reduce to 1.30 cm⁻¹ at the mole fraction χ_m (ET) = 0.13. Both the isotropic and anisotropic peak frequencies of CS stretching were found to shift to higher wavenumber when the concentrations are diluted, while the value of Δυ_nc goes on decreasing upon dilution. The absolute Raman cross section of carbonyl stretching was also measured, and their behavior was unusual (first increasing and then decreasing with the decrease of concentration). The experimental result shows that there may exist self‐association in the high concentration, and the main NCE mechanism may be due to the transition dipole–transition dipole coupling between the ET molecules. Copyright © 2015 John Wiley & Sons, Ltd.     

Stretching instability of helical springs

We show that when a gradually increasing tensile force is applied to the ends of a helical spring with sufficiently large ratios of radius to pitch and twist to bending rigidity, the end-to-end distance undergoes a sequence of discontinuous stretching transitions. Subsequent decrease of the force leads to steplike contraction, and hysteresis is observed. For finite helices, the number of these transitions increases with the number of helical turns but only one stretching and one contraction instability survive in the limit of an infinite helix. We calculate the critical line that separates the region of parameters in which the deformation is continuous from that in which stretching instabilities occur.     

Surface-Enhanced Infrared Spectral Investigations of 2,3-Bis(chloromethyl)anthracene-1,4,9,10-tetraone on Copper Nanoparticles

ABSTRACT

Surface-enhanced infrared (IR) absorption spectroscopic technique has been employed to investigate the orientation of 2,3-bis(chloromethyl)anthracene-1,4,9,10-tetraone (BCMAT) on copper nanoparticles (NPs). Copper NPs have been prepared by the chemical reduction method. The observed ring stretching modes show higher downshifts, broader bandwidths, and higher enhancement. The observed features in out-of-plane and in-plane CH deformation modes indicate that the BCMAT molecules may be adsorbed in a “flat-on” orientation on the copper NPs. The observed lower enhancement factor of the in-plane C?O deformation mode and C?O stretching mode and the higher enhancement factor of out-of-plane C?O deformation mode elucidate that the BCMAT molecules are adsorbed on the copper NPs in a “flat-on” orientation. All these observations show that BCMAT is adsorbed on copper NPs through the π-anthraquinone ring system in a “flat-on” orientation.     

乙烯基酯树脂光固化的拉曼光谱研究

文章利用理论计算(DFT,密度泛函理论)和实验两种方法得到了乙烯基酯树脂的拉曼光谱.通过对比分析,再结合相关文献,对其光谱的振动模式进行初步的指认,拉曼光谱中苯环平面内的变形振动在1598 cm-1、C=C的伸缩振动和C=O的伸缩振动分别在1628 cm-1和1702 cm-1.3007 cm-1和3062cm-1的振动归属于=C-H的伸缩振动和苯环上C-H的伸缩振动,而-C-H的伸缩振动在2800 cm-1~3000 cm-1.并且对比了可见光固化树脂固化前后的拉曼光谱图,可见光固化树脂的固化,主要由于1630cm-1C=C的交联反应产生.     

利用二维红外相关光谱研究胶原/透明质酸共混物的相互作用

以胶原/透明质酸共混物中透明质酸的含量为外扰,利用二维红外相关光谱法研究了胶原/透明质酸共混物的构象变化及它们之间的相互作用.研究发现,1694,1524与1241 cm-1归属于胶原酰胺带的C=O对称伸缩振动、N-H摇摆与N-H面内变形振动峰之间存在同步正交叉峰,表明随着透明质酸组分的增加,胶原的链段构象发生了变化.当胶原/透明质酸共混体系中透明质酸含量由0增至50%时,1045cm-1归属于透明质酸的C-OH伸缩振动峰与1694 cm-1归属于胶原C=O对称伸缩振动峰存在同步负交叉峰,表明透明质酸的O-H与胶原分子的C=O之间形成了氢键;当透明质酸含量从50%增至90%时,1045 cm-1的同步峰几乎消失,而在φ(1694,1524),φ(1694,1241),φ(1524,1241)出现的正交叉峰反而增强,说明透明质酸的O-H不再与胶原形成氢键,而是透明质酸的C=O与胶原分子的N-H之间形成氢键,致使胶原构象发生了变化.     

Denaturation transition of stretched DNA

We generalize the Poland-Scheraga model to consider DNA denaturation in the presence of an external stretching force. We demonstrate the existence of a force-induced DNA denaturation transition and obtain the temperature-force phase diagram. The transition is determined by the loop exponent c, for which we find the new value c = 4 nu-1/2 such that the transition is second order with c = 1.85 < 2 in d = 3. We show that a finite stretching force F destabilizes DNA, corresponding to a lower melting temperature T(F), in agreement with single-molecule DNA stretching experiments.