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1.
采用密度泛函理论B3LYP/6-31+G*方法对含Y型均三嗪类衍生物的6个分子(Y1-Y6)进行几何构型优化,对其最优构型采用TD-DFT (TDB3 LYP/6-31+G*)计算电子吸收光谱,用有限场FF方法及自编程序计算三阶非线性光学(NLO)性质.结果表明,6个含Y型均三嗪类有机分子的三阶非线性光学系数γ值为1010数量级个原子单位(10-30 esu),显示出良好的三阶非线性光学性能.在其三支链的末端引入不同的推、拉电子基团(Y2→Y6),对其电子光谱和三阶非线性光学响应具有明显的影响.引入强供电子基团,γ增大幅度较大,有利于改善体系的三阶非线性光学性质,从而可获得良好的非线性光学材料.  相似文献   

2.
采用密度泛函理论B3LYP/6-31+G(d,p)方法对二聚α、β-并三噻吩衍生物的15个分子(a~g2)进行几何构型优化,对其最优构型采用TD-DFT(TDB3LYP/6-31+G(d))计算电子吸收光谱,用有限场FF方法及自编程序计算三阶非线性光学(NLO)性质.计算结果表明,在乙烯分子(反式)两侧分别引入α-并三噻吩、β-并三噻吩基团(c分子)比单纯引入相同的α-并三噻吩(a分子)或β-并三噻吩(b分子)基团,更有利于增大其三阶非线性光学(NLO)性能.在含乙烯桥二聚α、β-并三噻吩(母体分子)结构的末端,端接含C=C或C≡C的基团(如-C≡CH与-C=C(CN)_2),与端接吸电子基F原子或给电子基-N(CH_2CH_3)_2相比,能隙降值减小,最低能量吸收波长明显红移,其三阶NLO系数γ值达10~6数量级个原子单位(10~(-33)esu),显示出良好的三阶非线性光学性能,可设计成为性能良好的三阶非线性光学材料.  相似文献   

3.
在QCISD/6-311G*水平上研究了B+4分子的各种稳定构型. 首先通过从头计算优化出可能的稳定构型, 再通过振动频率的计算判断所得构型是局部极小或鞍点. 同时讨论了Jahn-Teller效应. 通过比较发现从头计算得到的各种构型与群论的结果一致, 并得出一些文献中报道的构型实际上是鞍点. 首次报道了非平面的C2v 构型.  相似文献   

4.
采用密度泛函理论B3LYP/6-31+g(d)方法对二聚α、β-并三噻吩衍生物的18个分子(a~j2)进行几何构型优化,对其最优构型采用TD-DFT(TDB3LYP/6-31+g(d))计算电子吸收光谱,用有限场FF方法及自编程序计算二阶非线性光学(NLO)性质。计算结果表明,增加共轭链的含乙烯桥的二聚并三噻吩比不含乙烯桥者,βμ(或β0)大1.6—5.3倍;在含乙烯桥二聚α、β-并三噻吩分子(母体分子)末端引入含C=C或C≡C的基团(如-C≡CH与-C=C(CN)_2),比引入强供电子基团(如-N(CH_2CH_3)_2)、单纯吸电子基(如F原子)βμ(或β0)更大;尤其是端接-C=C(CN)2基团的二聚α、β-并三噻吩衍生物,其βμ(或β0)值为104数量级个原子单位(10-29esu),与母体分子相比βμ增大4.8~19.6倍,更有利于改善体系的二阶非线性光学性质,从而可获得良好的非线性光学材料.  相似文献   

5.
采用密度泛函理论B3LYP/6-31+g(d,p)方法对二聚α、β-并三噻吩衍生物的15个分子(a~g2) 进行几何构型优化,对其最优构型采用TD-DFT(TDB3LYP/6-31+g(d))计算电子吸收光谱,用有限场FF方法及自编程序计算三阶非线性光学(NLO)性质。计算结果表明,在乙烯分子(反式)两侧分别引入α-并三噻吩、β-并三噻吩基团(c分子)比单纯引入相同的α-并三噻吩(a分子)或β-并三噻吩(b分子)基团,更有利于增大其三阶非线性光学(NLO)性能。在含乙烯桥二聚α、β-并三噻吩 (母体分子)结构的末端,端接含C=C或C≡C的基团(如-C≡CH与-C=C(CN)2),与端接吸电子基F原子或给电子基-N(CH2CH3)2相比,能隙降值减小,最低能量吸收波长明显红移,其三阶NLO系数  值达106数量级个原子单位(10-33 esu),显示出良好的三阶非线性光学性能,可设计成为性能良好的三阶非线性光学材料。  相似文献   

6.
采用密度泛函理论B3LYP/6-311+g(d,p)方法对含苯乙烯桥侧链均三嗪类衍生物的8个分子(Y1-Y8)进行几何构型优化,对其最优构型采用TD-DFT(TDB3LYP/6-311+g(d,p)),计算电子吸收光谱,用有限场FF方法及自编程序计算二阶非线性光学(NLO)性质。结果表明,8个分子的μ(或0)值为104数量级个原子单位(10-29 esu),显示出良好的二阶非线性光学性能。在其三支链的末端引入强供电子基团(如-N(CH3)2或-N(CH2CH3)2)比引入弱供电子基团及吸电子基团,更有利于改善体系的二阶非线性光学性质,从而可获得良好的非线性光学材料。  相似文献   

7.
采用密度泛函理论B3LYP/6-31+G*方法对含Y型均三嗪类衍生物的6个分子(Y1-Y6)进行几何构型优化,对其最优构型采用TD-DFT(TDB3LYP/6-31+G*)计算电子吸收光谱,用有限场FF方法及自编程序计算三阶非线性光学(NLO)性质。结果表明,6个含Y型均三嗪类有机分子的三阶非线性光学系数g值为1010数量级个原子单位(10-30 esu),显示出良好的三阶非线性光学性能。在其三支链的末端引入不同的推、拉电子基团(Y2→Y6),对其电子光谱和三阶非线性光学响应具有明显的影响。引入强供电子基团,g增大幅度较大,有利于改善体系的三阶非线性光学性质,从而可获得良好的非线性光学材料。  相似文献   

8.
本文采用Gaussian03 B3P86方法,在6-311 G(3d2f)基组水平上,对S3分子进行几何优化理论计算,计算结果表明S3分子基态1A1最稳定的构型为C2V构型,其离解能为10.8372 eV,能量最小值为-1193.19946 a.u.,计算还得到了谐振频率、力常数,计算结果与实验值符合得很好.在此基础上利用多体展式理论方法得到了S3分子的解析势能函数和等值势能图,势能函数正确反映了S3分子的构型与能量变化.  相似文献   

9.
利用从头算HF方法在6 31G 基组水平下,全优化计算了1,3 取代方酸衍生物体系Sq1~Sq12的分子 几何和优化构型下的电子结构.以优化后的构型为基础,应用CIS/6 31G 方法计算了电子光谱.同时应用从头算 CPHF/6 31G 方法和半经验FF/AM1、FF/PM3、FF/MNDO有限场方法计算了分子的二阶非线性光学系数,并对 这四种计算方法的结果进行了系统的比较.结果表明,1,3 取代方酸衍生物的二阶非线性光学系数(β0)受五员 杂环的影响较大,引入吡咯、噻唑和口恶唑五员杂环能提高其β0,含两个杂原子的五员环与方酸碳四员环相连的位 置对β0也有很大的影响.  相似文献   

10.
本文用B3LYP方法,在6-31G*基组水平上对2,3,7,8-TCDD分子的构型进行了优化,得到它的稳定构型为平面型,具有D2h对称性。在优化构型的基础上计算了红外光谱和Raman光谱,并进行了振动分析。  相似文献   

11.
The nonlinear optical (NLO) semiorganic crystals barium thiourea chloride (BTC), bis(thiourea)barium chloride (BTBC) and barium(tetrakisthiourea) chloride (BTTC) were grown by the slow evaporation technique. FT‐Raman and IR spectra of the crystallized NLO materials were recorded and analyzed. The equilibrium geometry, bonding features and harmonic vibrational wavenumbers were investigated with the help of B3LYP density functional theory (DFT) method. From the optimized geometry, the decrease in C N bond length indicates the charge delocalization over the region of the molecules. Lengthening of CS bond and the deviation of CS···Cl angles clearly show the coplanarity of the amide planes of the complexes. The lowering of highest occupied molecular orbital (HOMO) and lowest unoccupied molecular orbital (LUMO) energy gap appears to be the cause for its enhanced charge transfer interactions. Copyright © 2011 John Wiley & Sons, Ltd.  相似文献   

12.
13.
具有反演对称中心的硅单晶在电场作用下体内的反演对称中心消失,因而理论上应产生偶数阶非线性极化率。从理论上根据矢量与张量的作用,利用(eχf2f)=χ(3).E这一关系和张量变换理论系统地阐述了硅材料在内建电场或外加电场的作用下,具体在方向分别沿[111][、110]和[001]的电场作用下,得到的等效二阶极化率张量(eχf2f)分别与C3v、C2v和C4v点群的二阶极化率张量具有相同的形式,说明在物理性质方面,硅的对称性由Oh群在相应方向电场作用下分别被降低为C3v、C2v和C4v群,因此应该具有相应对称性晶体的二阶非线性光学性质;提出了电场E沿任意方向时硅的等效二阶极化率张量e(χf2f)的计算方法,对研究硅材料和其他具有反演对称中心材料的场致二阶非线性光学性质实验具有指导意义。  相似文献   

14.
Sets of parton distribution functions (PDFs) of the proton are reported for the leading (LO), next-to-leading (NLO) and next-to-next-to-leading-order (NNLO) QCD calculations. The parton distribution functions are determined with the HERAFitter program using the data from the HERA experiments and preserving correlations between uncertainties for the LO, NLO and NNLO PDF sets. The sets are used to study cross-section ratios and their uncertainties when calculated at different orders in QCD. A reduction of the overall theoretical uncertainty is observed if correlations between the PDF sets are taken into account for the ratio of \(WW\) di-boson to \(Z\) boson production cross sections at the LHC.  相似文献   

15.
Solid-state nuclear magnetic resonance (NMR) spectroscopy is employed for the first time on urea and thiourea inclusion compounds (UICs and TICs) containing branched alkyl chains. In the present work,2H and13C NMR as well as X-ray diffraction studies of two selectively deuterated 2-methylhexadecanes in UIC and TIC are presented. An analysis of the derivedT 1 data reveals significant differences between UICs and TICs, which can be attributed to differences in the motional features of the guest species. It is found that four different motional contributions have to be considered, namely, chain rotation, chain wobbling,trans-gauche isomerization and methyl group rotation. 2-Methylhexadecane in UIC exists in an almost all-trans conformation (gauche amount not more than 5%) and undergoes fast chain rotation (6-site jump process, activation energyE A=16.7 kJ/mol). The analysis of the2H NMR spectra of 2-methylhexadecane-1,1′,2-d7 in urea proves that the branched chain end exists in an eclipsed conformation. TheT 1 data of 2-methylhexadecane-3-d2 in thiourea can be reproduced by an overall rotation (E A=9.8 kJ/mol) and atrans-gauche isomerization with torsional jumps around the C-3-C-4 bond (E A=11.0 kJ/mol,gauche population=15%). As for the corresponding UIC, the2H NMR spectra of 2-methylhexadecane-1,1′,2-d7 in TIC can be only explained by the existence of an eclipsed conformation at the branched chain end.  相似文献   

16.
The developments of nonlinear optical (NLO) crystals in the last decade are reviewed from two aspects. In the theoretical part, on the ab initio plane-wave pseudopotential energy method, calculation of the optical responses, including the second harmonic generation coefficients, a computer-program package, and a real-space atom-cutting method are described and employed to evaluate the degree of approximation of the anionic group theory for nonlinear optical crystals. The ab initio method combined with the anionic group theory gives much more insight into the understanding of the relationship between the optical responses and microscopic structures of NLO crystals, borate-based NLO crystals in particular. In the experimental part, we describe how to use the anionic group theory method and an experimental evaluation system to develop a series of borate-based UV-NLO crystals such as KBe2BO3F2 (KBBF) and K2Al2B2O7 (KABO). The capability of these new UV-NLO crystals in producing deep-UV harmonic output is evaluated and determined. Finally, recent advances in the generation of deep- and vacuum-UV harmonic output with these new NLO crystals are reported. PACS 42.65.Ky; 42.70.Mp  相似文献   

17.
The outer electronic levels of glycine, alanine, glycine ethyl ester, urea, and thiourea have been investigated by means of photoelectron spectroscopy using He I (584 Å) and He II (304 Å) radiation and CNDO/2 molecular orbital calculations. In the amino acids the molecular orbital (MO) ordering ha been found to be [σ core and carbonyl π > a″(O) a′(O) > a″(N)] with a first ionization potential of ~8.8 eV. Glycine and alanine are foun to exist as the undissociated amino carboxylic acids rather than zwitterions in the high temperature vapor. In urea the three lowest energy molecular o are near-degenerate [σ(4b1) ~ π(1a2) ~ π(2b2)] while in thiourea only the two lowest energy MO's are near-degenerate [π(1a2 σ(4b1) ~ π(2b2)]. The first ionization potentials of urea and thiourea are 9.7 and 7.9 eV respectively.  相似文献   

18.
An approximation method based on Regge behavior is presented. This new method relates the reduced cross section derivative and the structure function Regge behavior at low x. With the use of this approximation method, the C and λ parameters are calculated from the HERA reduced cross section data taken at low-x. Also, we calculate the structure functions F2(x,Q2) even for low-x values, which have not been investigated. To test the validity of calculated structure functions, we find the gluon distribution function in the Leading order approximation based on Regge behaviour of structure function and compare to the NLO QCD fit to H1 data and NLO parton distribution function.  相似文献   

19.
In PramanaJ. Phys.75, 683 (2010), Gunasekaran et al reported that they have grown the nonlinear optical crystals, urea thiourea mercuric chloride (UTHC) and urea thiourea mercuric sulphate (UTHS). We argue that UTHC and UTHS are dubious crystals and are not what the authors propose.  相似文献   

20.
A theoretical model suitable for calculating infrared absorption-edges of molecular nonlinear optical (NLO) crystals is introduced from high-level calculations of molecular vibrational spectra. The model is useful for elucidating the relationship between the molecular vibration and macroscopic absorption edges on the IR side of organic nonlinear optical crystals. The first-principle ab initio method carries out the calculations of IR absorption-edges of several typical molecular NLO crystals. These molecular NLO crystals include urea, 2-methyl-4-nitroaniline (MNA), meta-dinotrobenzene (MDNB), 3-methyl-4-methooxy-4-nitrostilbene (MMONS), and 3-hydroxyl-4-nitrostilbene (HMONS). The calculated results are compared with the measurements and good agreement is found between them. The experimentally unknown values of IR absorption-edges of some new synthesized crystals are predicted. The theoretical analyses of the structural origins of IR absorption cut-offs are discussed. The results are helpful for the molecular simulation and design of potential infrared molecular NLO crystals. Received: 9 April 2002 / Accepted: 18 July 2002 / Published online: 28 October 2002 RID="*" ID="*"Corresponding author. Fax: +86-591/3714946, E-mail: wkc@ms.fjirsm.ac.cn  相似文献   

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