共查询到20条相似文献,搜索用时 968 毫秒
1.
2.
3.
4.
ResonantFluorescenceofaΛtypeDegenerateQuantumbeatThrelevelAtomCAOZhuoliang(DepartmentofPhysics,AnhuiUniversity,Hefei230039... 相似文献
5.
6.
SUN Changyou 《Chinese Journal of Lasers》1996,5(2):129-136
TheSqueezingOperatorandtheSqueezedStatesof"Superspace"¥SUNChangyou(DepartmentofPhysics,HeiheTecher'sCollege,Heihe164300)MAAiq... 相似文献
7.
《Chinese Journal of Lasers》1996,(6)
AnalyticSubjectIndextoVolumeBS,(1996)LASERDEVICESPUlsewidthcharacteristicsofmode-lockedTi:sapphirelaserwithringcaavityKerr-le... 相似文献
8.
拉曼光活性(ROA)经典理论模型研究马树国吴国祯(清华大学物理系北京100084)AClasicalTheoryfortheRamanOpticalActivityMaShuguo,WuGuozhen(DepartmentofPhysics,Tsin... 相似文献
9.
10.
拉曼光谱在医学上的应用(Ⅱ)余国滔(北京大学生命科学学院北京100871)BiomedicalApplicationsofRamanSpectroscopy(Ⅱ)YueKwokto(ColegeofLifeSciences,PekingUnivers... 相似文献
11.
ZHAO Zhen-Min ZHANG Qi-Ren GAO Chun-Yuan 《理论物理通讯》2006,46(3):541-544
The potential energy surface of H(13) proton in base cytosine of the DNA molecules is calculated at the Caussian 98 MP2/6-311C(d,p) level. Two potential wells are found. One corresponds to the normal cytosine, while the other corresponds to its trans-imino tautomer. The estimated tunneling probability of the H(13) proton from one well to another well shows that the life time of the proton staying in one of these wells is about 600 yrs. It is too long to let tautomers of cytosine be in thermodynamical equilibrium in a room temperature gas phase experiment. 相似文献
12.
The potential energy surface of H(13) proton in base cytosine of the DNA molecules is calculated at the Gaussian 98 MP2/6-311G(d,p) level. Two potential wells are found. One corresponds to the normal cytosine, while the other corresponds to its trans-imino tautomer. The estimated tunneling probability of the H(13) proton from one well to another well shows that the life time of the proton staying in one of these wells is about 600 yrs. It is too long to let tautomers of cytosine be in thermodynamical equilibrium in a room temperature gas phase experiment. 相似文献
13.
《Current Applied Physics》2018,18(2):133-140
In this article, the adsorption of cytosine and guanine molecules on the surface of Cr-doped C20 fullerene (C19Cr) and Ni-doped C20 fullerene (C19Ni) are studied using first-principles density functional theory (DFT) calculations. In order to thoroughly comprehend the influences of the molecules on the metal-fullerene complexes, the geometric parameters, the binding energies, transferred charges, the magnitude of dipole moments, thermochemical parameters, frontier molecular orbitals, and the global indices of activities are calculated. The results highlighted that the interactions of both cytosine and guanine molecules with metal-fullerene complexes are highly exothermic, suggesting that these molecules might be chemisorbed on their adsorbents. The C19Cr exhibits a better adsorption behavior toward the molecules compared to C19Ni, and cytosine has the higher binding energies with metal-fullerene complexes in comparison with guanine. Further analyses showed that the C19Cr experiences significant changes in its electronic properties upon adsorption of the cytosine molecule. However, the small variations in the electronic properties of C19Ni after complexation with guanine indicate that this complex is not sensitive to the guanine. Furthermore, the results of frontier molecular orbital reveal the strong (moderate) interactions between the C19Cr with the cytosine (guanine) molecule and moderate (weak) interactions between the C19Ni with the cytosine (guanine) molecule. Therefore, the C19Cr and C19Ni have moderate sensitivities to cytosine and guanine molecules. More excitingly, our findings divulge promising potential of the Cr-fullerene complex as a biochemical adsorbent for cytosine. 相似文献
14.
15.
运用Gaussian98 MP2/6 311G(d, p)级的从头计算法计算了DNA分子中胞嘧啶碱基中H13质子的势能曲面。 发现有两个势阱: 其中一个对应正常的胞嘧啶, 而另一个则对应它的顺式亚胺式互变异构体。 质子在这两个势阱的束缚对热扰动是稳定的。 质子在势阱中像单摆一样绕着离它最近的氮原子摆动, 还可以远离氮原子与其它碱基形成氢键。 估算出的H13质子从一个势阱到另一个势阱的穿透几率表明质子呆在其中一个势阱中的寿命大约是6×102 a, 这使胞嘧啶和它的顺式亚胺式互变异构体在室温气相实验中远不能达到热平衡。 对这些结果的生物学意义作了讨论。 The potential energy surface of the H13 proton in base cytosine of theDNA molecules is calculated ab initio at the Gaussian98 MP2/6 311G(d, p) level. Two potential wells are found. One corre sponds to the normal cytosine, while the other corresponds to its imino tautomer. The bindings of the proton in these wells are stable enough against the thermo disturbance. The motions of the proton in these wells are oscillations around the nearest nitrogen atom like the pendulum, and may move far away from the nitrogen atom to form the hydrogen bond with other bases. The estimated tunneling probability of the H13 proton from one well to another well shows that the life time of the proton staying in one of these wells is about 6×102 a. It is too long to let tautomers of cytosine be in thermodynamical equilibrium in a room temperature gas phase experiment. The biological significance of these results is discussed. 相似文献
16.
17.
Weightman P Dolan GJ Smith CI Cuquerella MC Almond NJ Farrell T Fernig DG Edwards C Martin DS 《Physical review letters》2006,96(8):086102
It is demonstrated using reflection anisotropy spectroscopy that the adsorption of cytosine and cytidine -monophosphate at the Au(110) 1 x 2/electrolyte interface gives rise to ordered structures in which the base is oriented vertical to the surface and parallel to the [110] axis of the Au(110) plane. 相似文献
18.
Since nucleobase-functionalized carbon nanotubes (CNTs) are important in the biological applications; the junction of a pair of CNTs through a bridging cytosine linkage is investigated based on density functional theory (DFT) calculations. In the exact model of study, the CNTs are bound to N1 and C5 atomic sites of cytosine to make possible the CNT–cytosine–CNT model. To systematically investigate the purpose, the models of original CNT, original cytosine, and primary models of cytosine–CNT in which one CNT is only bound to N1 or C5 atomic site of cytosine are also considered. The results of dipole moments and binding energies indicated that the CNT–cytosine–CNT model is the most stable one among all three possible models cytosine-functionalized CNT. The values of energy gaps indicated that the conducting properties of primary cytosine–CNT models are not changed referring to the original CNT but better conductivity could be observed for the CNT–cytosine–CNT model. The values of evaluated quadrupole coupling constants indicated that the electronic densities of nitrogen and oxygen atoms of cytosine detect notable affects during the functionalization processes by the zigzag CNTs and the oxygen atom of CNT–cytosine–CNT model could be proposed as the most proper interacting site of cytosine among other functionalized zigzag models and also the original cytosine. However, the changes of quadrupole coupling constants for the atoms of cytosine are almost negligible during the functionalization processes by the armchair CNTs. 相似文献
19.
DNA碱基分子胞嘧啶和胸腺嘧啶的太赫兹光谱研究 总被引:1,自引:0,他引:1
利用太赫兹时域光谱技术获得了DNA碱基分子胞嘧啶和胸腺嘧啶在0.1―3.5 THz的特征吸收谱,发现胞嘧啶在2.53 THz的特征吸收细节信息。采用考虑了周期性边界条件的赝势平面波密度泛函方法对胞嘧啶分子晶体进行了结构优化和晶格动力学计算,模拟重现其太赫兹特征吸收光谱,并成功辨识了胞嘧啶在0.1―3.5 THz的所有特征吸收峰。研究结果表明,这些重要的生物分子在太赫兹频段表现出鲜明的光谱特性,胞嘧啶分子3.5 THz以下的吸收特性均来源于由分子间氢键支配的外振动模式。 相似文献
20.
We propose a mechanism of DNA single strand breaks
induced by low-energy electrons. Density functional theory calculations have
been performed on a neutral, hydrogenated, and/or negatively charged
nucleotide of cytosine in the gas phase to identify barriers for the
phosphate-sugar O–C bond cleavage. Attachment of the first excess electron
induces intermolecular proton transfer to cytosine. The resulting neutral
radical of hydrogenated cytosine binds another excess electron, and the
excess charge is localized primarily on the C6 atom. A barrier encountered
for proton transfer from the C2’ atom of the adjacent sugar unit to the C6
atom of cytosine is 3.6 and 5.0 kcal/mol, based on the MPW1K and B3LYP
electronic energies corrected for zero-point vibrations, respectively. The
proton transfer is followed by a barrier-free sugar-phosphate C–O bond
cleavage. The proton transfer is impossible for the neutral nucleotide, as
there is no local minimum for the product. In the case of anionic and
hydrogenated nucleotides the same barrier determined at the B3LYP level is
as large as 29.3 and 22.4 kcal/mol respectively. This illustrates that the
consecutive hydrogenation and electron attachment make the nucleotide of
cytosine susceptible to a strand break. The rate of the C–O bond cleavage in
the anion of hydrogenated nucleotide of cytosine is estimated to be ca.
1010 s-1. The proposed mechanism proceeds through bound anionic
states, not through metastable states with finite lifetimes and discrete
energy positions with respect to the neutral target. The results suggest
that
at least for DNA without hydration
even very low-energy electrons may cleave the DNA backbone. 相似文献