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设计并合成了一种新型的非线性材料分子,2-二氰基甲叉-3-氰基-4-[2-N,N-二羟基乙基氨基苯乙烯基]-5,5-二甲基-2,5-二氢呋喃.用红外光谱、核磁共振氢谱和元素分析对其进行了表征,用X射线单晶衍射仪测定了其晶体结构,该晶体属于三斜晶系,空间群为P-1,晶胞参数分别为a=9.5364(12)nm,b=10.1030(15)nm,c=13.599(2)nm,α=91.306(2)°,β=102.046(3)°,γ=117.149(3)°,Dc=1.148 g/cm3,Z=2,F(000)=412,V=1129.7(3)nm3.

参考文献

[1] Arder S R;Cheng L T;Tiemann B C et al.Large First Hyperpolarizabilities in Push-pull Polyenes by Tuning of the Bond Length Alternation and Aromaticity[J].Science,1994,263:511-514.
[2] Zhu W H;Wu G S .An Ab Inito Study on the First-an Third-order Polarizabilities of the Octupolar Heteroaromatic-substituted Triazines[J].Journal of Physical Chemistry A,2002,106:7216-7221.
[3] Yanagi K;Kobayashi T;Hashimoto H .Origin of Transition Dipolo-moment Polarizability and Hyperpolarizability in Hydrazones[J].Physical Review,2003,B67:115122.
[4] Dalton LR. .Rational design of organic electro-optic materials [Review][J].Journal of Physics. Condensed Matter,2003(20):R897-R934.
[5] He MQ.;Leslie TM.;Sinicropi JA.;Garner SM.;Reed LD. .Synthesis of chromophores with extremely high electro-optic activities. 2. Isophorone- and combined isophorone-thiophene-based chromophores[J].Chemistry of Materials,2002(11):4669-4675.
[6] Mingqian He;Thomas Leslie;Sean Garner;Michael DeRosa;Jeffery Cites .Synthesis of New Electrooptic Chromophores and Their Structure-Property Relationship[J].The journal of physical chemistry, B. Condensed matter, materials, surfaces, interfaces & biophysical,2004(25):8731-8736.
[7] He MQ.;Leslie TM.;Sinicropi JA. .alpha-Hydroxy ketone precursors leading to a novel class of electro-optic acceptors[J].Chemistry of Materials,2002(5):2393-2400.
[8] Sheldrick,G M.SHELXL-97.Program for Crystal Structure Determination[M].Germany:University of G(o)ttingen,1997
[9] Sheldrick G M.SADABS,Siemens Area Detector Absorption(and Other)Correction[M].Germany:University of Gttingen,1997
[10] 陆荣健.1-芳胺羰基-3-苄硫基-4-乙氧羰基(或氰基)-5-氨基吡唑的合成及生物活性[J].高等学校化学学报,1996(08):1231.
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