Iwaura Rika, Ohnishi-Kameyama Mayumi, Iizawa Tomohiko
National Food Research Institute, National Agriculture and Food Research Organization, 2-1-12 Kannondai, Tsukuba, Ibaraki, 305-8642, Japan.
Chemistry. 2009;15(15):3729-35. doi: 10.1002/chem.200802537.
The thymidylic acid appended anthracene dye 2,6-bis[5-(3'-thymidylic acid)pentyloxy]anthracene (1) was synthesized, and the self-assembly of 1 and the binary self-assembly of 1 with a complementary single-stranded 20-meric oligodeoxyadenylic acid (dA(20)) were performed in 0.1 x TE buffer solution (i.e., 1.0 x 10(-3) M Tris-HCl, 1.0 x 10(-4) M ethylenediaminetriacetic acid (EDTA)). The characteristic J-band, small Stokes shift (6 nm), Cotton effect, and helical nanofibers 5.1 nm in diameter are observed in UV/Vis, fluorescence, and circular dichroism (CD) spectroscopies and atomic force microscopy (AFM) measurements for the binary self-assembly of 1 and dA(20) in aqueous solution. These observations revealed that the helical J-aggregates, in which the short-axis transition dipoles of the anthracene moieties are aligned in a head-to-tail fashion, are formed from the binary self-assembly of 1 and dA(20). The UV/Vis absorption and CD band of the anthracene L(a) region were found to be strongly dependent on temperature and showed cooperative changes for the binary self-assembly of 1 and dA(20). The self-assembly of the single-component 1 produced right- and left-handed helical nanofibers with diameters ranging from 4.0 to 10 nm. In contrast, for the binary self-assembly, the UV/Vis and fluorescence spectra showed no J-band and the Stokes shift was at approximately 107 nm for the single-component 1 in aqueous solution. In addition, the binary self-assembly of 1 and noncomplementary single-stranded 20-meric oligothymidylic acid (dT(20)) showed a small J-band and the J-band disappeared at 50 degrees C upon heating. On the basis of these observations, we concluded that thymine-adenine base-pair formation induced supramolecular helical J-aggregates in the binary self-assembly of 1 and dA(20) in aqueous solutions.
合成了连接胸苷酸的蒽染料2,6 - 双[5 - (3'-胸苷酸)戊氧基]蒽(1),并在0.1×TE缓冲溶液(即1.0×10⁻³ M Tris - HCl,1.0×10⁻⁴ M乙二胺三乙酸(EDTA))中进行了1的自组装以及1与互补的20聚体寡聚脱氧腺苷酸(dA(20))的二元自组装。在紫外可见光谱、荧光光谱、圆二色光谱(CD)以及原子力显微镜(AFM)测量中,观察到了1与dA(20)在水溶液中的二元自组装具有特征性的J带、小斯托克斯位移(6 nm)、科顿效应以及直径为5.1 nm的螺旋纳米纤维。这些观察结果表明,蒽部分的短轴跃迁偶极以头对头方式排列的螺旋J聚集体是由1与dA(20)的二元自组装形成的。发现蒽L(a)区域的紫外可见吸收和CD带强烈依赖于温度,并且对于1与dA(20)的二元自组装呈现协同变化。单一组分1的自组装产生了直径范围为4.0至10 nm的右手和左手螺旋纳米纤维。相比之下,对于二元自组装,紫外可见光谱和荧光光谱没有显示J带,并且单一组分1在水溶液中的斯托克斯位移约为107 nm。此外,1与非互补的20聚体寡聚胸苷酸(dT(20))的二元自组装显示出小的J带,并且加热至50℃时J带消失。基于这些观察结果,我们得出结论,胸腺嘧啶 - 腺嘌呤碱基对的形成在水溶液中1与dA(20)的二元自组装中诱导了超分子螺旋J聚集体。