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1.
采用量子化学UPBE1PBE结合有限场(FF)方法,对系列TTF+?-π共轭桥-6-氧四联氮阳离子双自由基体系的稳定性,极化率αs和第一超极化率βtot进行研究.结果表明,TTF+?-6-氧四联氮阳离子双自由基引入共轭桥后,随体系共轭性增强,αs和βtot值均增大(体系2S的βtot值除外).自旋多重度和构象对双自由基体系的极化率和第一超极化率都有影响,双自由基体系由单重态转变为三重态时,极化率减小,而第一超极化率明显增大.以体系2为例,在单重态时αs和βtot值随构象变化较小,而三重态时αs和βtot值随二面角θ1和θ2的增加而减小.  相似文献   

2.
以实验合成的联吖叮氮氧自由基分子为母体, 设计了7个自由基分子. 采用密度泛函理论(DFT) UB3LYP/6-31g(d,p)方法对这些自由基分子不同自旋态的稳定性和非线性光学(NLO)系数进行计算. 结果表明, 联吖叮氮氧自由基分子及其衍生物三重态为稳定基态, 符合自旋极化规则. 引入给吸电子取代基使自由基体系的极化率αs与二阶超极化率γs值有所增大, 且基团的给吸电子能力越强, αs和γs值增加越明显; 对于一阶超极化率βtot, 自由基体系处于单重态时, 取代基的影响较大. 所有自由基分子三重态的NLO系数都小于单重态, 表明可以通过控制体系的自旋多重度来调节体系的NLO性质.  相似文献   

3.
采用量子化学UMP2/6-31G(d,p)方法优化双噻唑苯二聚体自由基分子的几何结构,以0.05nm为单位步长拉长与缩短2分子片之间的距离,选取5个点,采用DFTUB3LYP/6-31G(d,p)方法,对双噻唑苯二聚体自由基分子的极化率和二阶超极化率进行理论计算.结果表明,自由基体系的单重态为相对稳定状态.在完全重叠的体系中,在单、三重态时极化率都随着2分子片间距离的增大而增加;三重态时二阶超极化率的绝对值随着2分子片间距离的增大而增大.部分重叠的体系,单重态时极化率随2分子片距离的增大而减小;三重态时,二阶超极化率的绝对值随着2分子片间距离的增大而增大.  相似文献   

4.
采用密度泛函理论(DFT)结合有限场(FF)方法,对不同共轭桥连接的四氰代二甲基苯醌(TCNQ)开壳层和闭壳层电子态的非线性光学(NLO)系数进行计算,并以乙烯桥为例讨论共轭链长度与NLO性质的关系.结果表明:开壳层体系的极化率和二阶超极化率值都大于闭壳层体系,且共轭桥的共轭性越强,体系的极化率和二阶超极化率越大;在自由基体系中,单重态的二阶超极化率随双自由基成分y和自旋多重度的增加而增大.体系的共轭链增长,BLA(BondLength Alternation,共轭分子中相邻单、双键键长差的平均值)逐渐减小,双自由基成分y逐渐增大,体系的二阶超极化率也逐渐增大.  相似文献   

5.
采用密度泛函理论(DFT)的UB3LYP(B3LYP)/6-31+G**方法对双咪唑苯和双三咪唑苯双自由基及其衍生物几何结构进行优化,并结合有限场(FF)方法计算这些体系的非线性光学(NLO)系数.结果表明,引入给、受体取代基都能使体系的极化率α和二阶超极化率γ增大.在双自由基体系中,引入给体NH2的α和γ值大于引入受体NO2的值,与闭壳层体系中结果相反.分析自由基成分和电荷对体系的二阶超极化率γ影响的结果表明,处于中间双自由基成分的分子比相似共轭性的闭壳层分子有更大的二阶超极化率γ;带电荷的双自由基体系引入给、受体之后,与中性自由基体系相比具有更大的二阶超极化率γ.  相似文献   

6.
采用密度泛函理论(DFT) UB3LYP方法, 在6-31g(d)水平上对2,2’-(1,2-乙炔基-4,1-亚苯基)双[4,4’,5,5’-四氢]咪唑氧自由基分子及其异构体的自旋耦合性质进行分析, 并结合有限场(FF)方法计算它们的非线性光学(NLO)系数, 以探讨咪唑氧环在共轭链不同位置时体系的自旋耦合规律和NLO系数. 结果表明, 所有体系基态自旋符合自旋极化规则, 它们的极化率随自旋多重度的增加而减小; 一阶超极化率因受分子对称性影响, 对称性不同其一阶超极化率的变化也不同; 二阶超极化率呈现随着自旋多重度的增加而增加的趋势. 从理论上探讨这些自由基分子自旋耦合规律与NLO活性的关系, 为有机自由基NLO材料的分子设计与实验研究提供一定的理论依据.  相似文献   

7.
SiCS分子结构及其稳定性的理论研究   总被引:5,自引:1,他引:4  
采用DFT,QCISD及CCSD(T)方法对单重态、三重态SiCS的分子体系势能面进行理论计算,在QCISD/6-311G(d)水平上得到由3个过渡态连接的5个稳定构型.经动力学及热力学分析均是稳定的三重态线型分子SiCS(31)、单重态线型分子SiCS(11)以及单重态的环状分子cSiCS(12).  相似文献   

8.
五元杂环分子超极化率的电子相关效应   总被引:2,自引:0,他引:2  
用有限场方法在HF和MP4水平上计算呋喃、吡咯和噻吩的极化率、一阶和二阶超极化率.结果表明,电子相关效应对各阶极化率,尤其是高阶极化率影响较大.MP2计算值较HF有显著改善,一阶超极化率的MP2,MP3和MP4计算值依次增大,二阶超极化率的MP2和MP4值相近,而MP3值小于MP2.呋喃、吡咯和噻吩的各阶极化率在各级微扰中均具有与HF水平上一致的相对大小顺序.  相似文献   

9.
采用密度泛函理论(DFT)方法对卟啉-碳硼烷-硼亚甲基二吡咯(BODIPY)三元化合物的几何结构、 吸收光谱及二阶非线性光学(NLO)特性进行计算分析. 结果表明, V型化合物的静态第一超极化率(βtot)大于相应直线型化合物, 且延长共轭链可提高体系的βtot. 分析体系的电子密度差分图得出, 化合物氧化还原态的电荷转移方式与本征态相比发生了改变, 从而使其二阶NLO性质发生明显变化. 含频第一超极化率计算结果表明, 在一定范围内频率对化合物有较小的色散效应. 因此, 通过延长二维化合物的共轭链及氧化还原反应, 可以有效调控其二阶NLO响应.  相似文献   

10.
有机-过渡金属配合物的三重态发光问题   总被引:1,自引:1,他引:0       下载免费PDF全文
近年来,随着OLED器件的发展,有关有机-过渡金属配合物的三重态发光问题受到人们广泛的关注。这不仅是与电致发光器件效率的提高相关联,同时也是一个在光物理研究中值得深入研究的课题.文章对有机-金属化合物激发态的能级分裂,以及发光三重态亚态的零场-分裂(ZFS)等进行了讨论,对具不同电子构型中心金属离子,例如八面体结构与平面四方形构型结构等与它们光物理行为间的关系进行了讨论.特别对这类体系的发光三重态在自旋轨道偶合作用(SOC)和构型相互作用(CI)的影响下,导致单重态与三重态的混合和促进从最低三重态到基态的发光跃迁进行了讨论.  相似文献   

11.
Equimolar copolymers of N-vinyl pyrrolidone with 1,1,1-3,3,3-hexafluoroisopropyl-α-fluoroacrylate were obtained by reversible addition-fragmentation chain transfer radical (RAFT) polymerization and by conventional radical polymerization (RAD). The copolymer conformation and compositional heterogeneity were analyzed by dynamic and static light scattering. RAFT copolymers of 41,000 ≤ M w  ≤ 68,000 g/mol were shown to adopt cylindrical all-trans conformation. RAD copolymer of higher molecular mass (Mw = 390,000 g/mol) exhibited less extended conformation, thus indicating that the statistical Kuhn segment is less than RAD copolymer length.  相似文献   

12.
The formation of an unprecedented macrocycles‐in‐a‐macrocycle (MIM) superstructure by reversible radical–radical association of a triphenylamine based monomer terminated with three dicyanomethyl radicals is presented. The reaction yield is nearly quantitative and the obtained macrocycle contains three small dimeric macrocycles according to X‐ray crystallographic analysis. The six monomer molecules are linked by nine long dynamic covalent C(sp3)?C(sp3) bonds that all adopt a gauche conformation. Such a conformation favors the formation of a MIM structure rather than a 2D network with an all‐anti conformation. Two enantiomers with left‐/ right‐handed chirality exist in the single crystals of the superstructure.  相似文献   

13.
Photopolymerization of methacrylic monomers yields samples with trapped radicals that are easily detected by electron paramagnetic resonance (EPR) spectroscopy. Despite its simplicity, there is no general agreement about the interpretation of this spectrum, in particular, about the role of methylene β protons. An extensive ENDOR study of the propagating radical in photopolymerized dimethacrylates has been carried out in order to obtain detailed information about methylene hyperfine couplings and, thus, about radical conformation. It is shown that literature models are not able to reproduce the ENDOR results and that only accurate fitting of ENDOR spectra obtained by saturating the EPR spectrum at different positions gives reliable information about radical conformation, thanks to the exploitation of conformational selectivity. It turns out that most radicals are in the minimum energy conformation, but any possible conformation is assumed by non negligible fractions of radical.  相似文献   

14.
用DFT,CASSCF和QCISD(T)方法6-31G*基组计算了构象对同位二取代乙烯双自由基体系基态自旋多重度及其稳定性的影响.结果表明,用DFT或CASSCF方法计算的单、三重态的能量差随自由基与乙烯间的二面角增加成不规则变化;用QCISD(T)方法计算的单、三重态的能量差随二面角的增加而逐渐降低,并呈规律性变化,说明QCISD(T)方法用于计算分子的磁性是可信的.对于同位二取代乙烯双自由基体系,无论双自由基旋转,还是单自由基旋转,高自旋基态稳定性随自由基与乙烯间二面角的增加而降低,只是降低的幅度不同,当二面角接近90°时,同位乙烯由具有平面或近似平面构象时强的铁磁耦合单元变成接近垂直平面构象时弱的反铁磁耦合单元或弱的铁磁耦合单元.  相似文献   

15.
A series of novel spiroadamantyl- and spirocyclical substituted pyranoquinolin-2-ones were synthesized and the conformation of the pyran ring was investigated. The free radical scavenging activity of the synthesized compounds was determined by their interaction with the stable free radical 1,1-diphenyl-2-picrylhydrazyl (DPPH). All compounds tested scavenged the DPPH radical and among them derivatives possessing extended conjugation showed the highest activity.  相似文献   

16.
We previously theorized that, since the stereoselectivity of anomeric radical reactions is significantly influenced by the kinetic anomeric effect, which can be controlled by restricting the conformation of the radical intermediate, the proper conformational restriction of the pyranose ring of the substrates would therefore make highly alpha- and beta-stereoselective anomeric radical reactions possible. This theory was based on our previous results of the anomeric radical reactions with d-xylose derivatives as the substrates. We herein report the anomeric radical deuteration reactions with the conformationally restricted 1-phenylseleno-d-glucose derivatives, 2g and 3g, restricted in a (4)C(1)-conformation by an O-cyclic diketal moiety, and 4g, 5g, 6g, 7g, and 8g, restricted in a (1)C(4)-conformation by bulky O-silyl protecting groups. The radical deuterations with Bu(3)SnD, using the (4)C(1)-restricted substrates 2g and 3g, afforded the corresponding alpha-products (alpha/beta = 98:2) highly stereoselectively, whereas the (1)C(4)-restricted substrate 6g, having a trigonal (sp(2)) carbon substituent, i.e., -CHO, at the 5-position, selectively gave the beta-products (alpha/beta = 0:100). Thus, the stereoselectivity was significantly increased by the conformational restriction and was completely inverted by changing the substrate conformation from the (4)C(1)-form to the (1)C(4)-form. On the other hand, the deuterations with the (1)C(4)-restricted substrates 4g and 5g showed that the 1,5-steric effect due to the tetrahedral carbon substituent (-CH(2)OTIPS or -CH(2)OH) at the 5-axial position dominantly prevented the hydride transfer from the beta-face competing with the kinetic anomeric effect. This study suggests that, depending on the restricted conformation of the substrates to the (4)C(1)- or the (1)C(4)-form, the alpha- or beta-products would be obtained highly stereoselectively via anomeric radical reactions of hexopyranoses.  相似文献   

17.
18.
An EPR study at 3 K of X-ray irradiated monofluoroacetamide does not reveal a radical anion species, despite the fact that the radical anion in trifluoroacetamide is stable at 77 K. This difference in stability has been found to be dependent on the conformation of the -CF3 group (eclipsed) versus the -CFH2 group (staggered). The eclipsed conformation permits effective σ-π hyperconjugation in stabilizing the radical anion. An INDO calculation of CF3CONH2? suggests that the radical site is pyramidal rather than planar with a non-planar angle of 32° and a dihedral angle for the eclipsed fluorine, relative to the nearly π-like orbital, of 30°.  相似文献   

19.
Far-UV photolysis of 4-thiothymidylyl(3'-5')thymidine led to the formation of three stable derivatives: one resulting from a combination between a 3'-end methylene radical and a 5'-end C(4) radical [4-(alpha-thyminyl) derivative] and two formed after a combination between a 3'-end methylene radical and a 5'-end C(6) radical [6-(alpha-thyminyl) derivative]. In the latter series, two stereochemical pathways took place during the reaction between the methylene and C(6) radicals. The major pathway occurred when the 5'-base glycosidic bond had an anti conformation leading to an S configuration of the C(6) Tp-end. The minor pathway, which had never been reported before in this series, involved a 5'-base in a syn conformation leading consequently to the R configuration at the C(6) Tp-end. The 5,6-dihydrothymine moiety of these two adducts presented a 5,6-trans diaxial substitution that resulted from the epimerization, at the 5,6-dihydropyrimidine 5-position, of a less stable cis-disubstituted intermediate.  相似文献   

20.
Aromatic sulfoxide radical cations have been generated by pulse radiolysis and laser flash photolysis techniques. In water (pulse radiolysis) the radical cations showed an intense absorption band in the UV region (ca. 300 nm) and a broad less intense band in the visible region (from 500 to 1000 nm) whose position depends on the nature of the ring substituent. At very low pulse energy, the radical cations decayed by first-order kinetics, the decay rate increasing as the pH increases. It is suggested that the decay involves a nucleophilic attack of H(2)O or OH(-) (in basic solutions) to the positively charged sulfur atom to give the radical ArSO(OH)CH(3)(*). By sensitized [N-methylquinolinium tetrafluoborate (NMQ(+))] laser flash photolysis (LFP) the aromatic sulfoxide radical cations were generated in acetonitrile. In these experiments, however, only the band of the radical cation in the visible region could be observed, the UV band being covered by the UV absorption of NMQ(+). The lambda(max) values of the bands in the visible region resulted almost identical to those observed in water for the same radical cations. In the LFP experiments the sulfoxide radical cations decayed by second-order kinetics at a diffusion-controlled rate, and the decay is attributed to the back electron transfer between the radical cation and NMQ(*). DFT calculations were also carried out for a number of 4-X ring substituted (X = H, Me, Br, OMe, CN) aromatic sulfoxide radical cations (and their neutral parents). In all radical cations, the conformation with the S-O bond almost coplanar with the aromatic ring is the only one corresponding to the energy minimum. The maximum of energy corresponds to the conformation where the S-O bond is perpendicular to the aromatic ring. The rotational energy barriers are not very high, ranging from 3.9 to 6.9 kcal/mol. In all radical cations, the major fraction of charge and spin density is localized on the SOMe group. However, a substantial delocalization of charge and spin on the ring (almost 50% for the 4-methoxy derivative and around 30% for the other radical cations) is also observed. This suggests some conjugative interaction between the MeSO group and the aromatic system that may become very significant when a strong electron donating substituent like the MeO group is present. The ionization energies (IE) of the 4-X ring substituted neutral aromatic sulfoxides were also calculated, which were found to satisfactorily correlate with the experimental E(p) potentials measured by cyclic voltammetry.  相似文献   

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