摩熵化学
数据库官网
小程序
打开微信扫一扫
首页 分子通 化学资讯 化学百科 反应查询 关于我们
请输入关键词

5''-ethynyl-[2,2';5',2'']terthiophene-5-carbaldehyde | 791111-24-5

中文名称
——
中文别名
——
英文名称
5''-ethynyl-[2,2';5',2'']terthiophene-5-carbaldehyde
英文别名
5-[5-(5-Ethynylthiophen-2-yl)thiophen-2-yl]thiophene-2-carbaldehyde;5-[5-(5-ethynylthiophen-2-yl)thiophen-2-yl]thiophene-2-carbaldehyde
5''-ethynyl-[2,2';5',2'']terthiophene-5-carbaldehyde化学式
CAS
791111-24-5
化学式
C15H8OS3
mdl
——
分子量
300.426
InChiKey
WZZUPEKSAJIIOV-UHFFFAOYSA-N
BEILSTEIN
——
EINECS
——
  • 物化性质
  • 计算性质
  • ADMET
  • 安全信息
  • SDS
  • 制备方法与用途
  • 上下游信息
  • 反应信息
  • 文献信息
  • 表征谱图
  • 同类化合物
  • 相关功能分类
  • 相关结构分类

计算性质

  • 辛醇/水分配系数(LogP):
    3.3
  • 重原子数:
    19
  • 可旋转键数:
    4
  • 环数:
    3.0
  • sp3杂化的碳原子比例:
    0.0
  • 拓扑面积:
    74.6
  • 氢给体数:
    0
  • 氢受体数:
    4

反应信息

  • 作为反应物:
    参考文献:
    名称:
    钌-噻吩基乙炔基钌配合物的设计与合成。声致非线性光学的新材料
    摘要:
    已经开发了一系列围绕不同长度的基于噻吩的π共轭间隔基构建的新的供体-π-受体钌钌系统。这些供体-π-受体生色团的线性和三阶非线性光学性质的比较表明,基于低聚噻吩的间隔基的延伸或进一步引入双键导致二噻吩基乙烯间隔基产生最大吸收的显着红移以及分子立方超极化性的显着增强。此外,对于掺入PMMA基质中的这些复合物的薄膜复合材料,还观察到了声诱发的第二谐波产生(AISHG),其值达到了迄今为​​止报道的最高值。
    DOI:
    10.1021/om049236s
  • 作为产物:
    描述:
    5-溴-5'-甲酰基-2,2':5'2'-三噻吩 在 bis-triphenylphosphine-palladium(II) chloride copper(l) iodide四丁基氟化铵三乙胺 作用下, 以 四氢呋喃 为溶剂, 反应 25.0h, 生成 5''-ethynyl-[2,2';5',2'']terthiophene-5-carbaldehyde
    参考文献:
    名称:
    χ(2) Grating in Ru Derivative Chromophores Incorporated within the PMMA Polymer Matrices
    摘要:
    We have found that Ru derivative chromophores incorporated into the PMMA polymer matrices might be considered as promising materials for optical poling. The maximally achieved effective second-order optical susceptibility for the wavelength 1.89 mum is about 1.94 pm/V. The investigated composites possess metastable trapping levels originating both from the d states of Ru and due to effective charge transfer due to the presence of pi-conjugated states. Because of incorporation of the chromophore into polymer matrices, we have revealed that the maximal susceptibility is observed at 5-6% of the chromophore in weighting units. The further increase of the second-order susceptibility is limited by the appearance of chromophore agglomerates substantially restraining second-order susceptibilities. The investigated composites possess long-lived chi((2)) grating, which decreases less than 76% after 600 min of laser treatment. The electrostatic field causes additional reanimation of the second harmonic generation during the decay regime. The electron microscopy pictures clearly confirm appearance of the chi((2)) grating.
    DOI:
    10.1021/jp048794h
点击查看最新优质反应信息

文献信息

  • Synthesis, photovoltaic performances and TD-DFT modeling of push–pull diacetylide platinum complexes in TiO<sub>2</sub> based dye-sensitized solar cells
    作者:Sébastien Gauthier、Bertrand Caro、Françoise Robin-Le Guen、Nattamai Bhuvanesh、John A. Gladysz、Laurianne Wojcik、Nicolas Le Poul、Aurélien Planchat、Yann Pellegrin、Errol Blart、Denis Jacquemin、Fabrice Odobel
    DOI:10.1039/c4dt00301b
    日期:——

    Five new Pt-containing dyes have been synthesised and characterised in the framework of DSSC applications.

    在DSSC应用的框架内,已合成并表征了五种新的含铂染料。
  • Second-order optical effects in organometallic nanocomposites induced by an acoustic field
    作者:A. Migalska-Zalas、B. Sahraoui、I. V. Kityk、S. Tkaczyk、V. Yuvshenko、J.-L. Fillaut、J. Perruchon、T. J. J. Muller
    DOI:10.1103/physrevb.71.035119
    日期:——
    Acoustically stimulated second-order optical effects in Ru-derivative nanocomposites were discovered. The alkynyl ruthenium derivatives were embedded in a polymethyl methacrylate (PMMA) polymer matrix. As second-order optical effects we studied second-harmonic generation (SHG) and linear electro-optics (LEO) phenomena. The physical insight of the effect observed consists in a coexistence of nanocofined chromophore levels and localized d states of ruthenium. A transverse acoustic field favors the occurrence of charge density noncentrosymmetry required for observation of the second-order optical effects, particularly SHG. We have found that acoustically induced SHG and LEO for fundamental YAB-Gd3+ laser light (lambda=1.76 mum) increases and achieves a maximum value at acoustic power density of about 1.45 W/cm(2). The values of the SHG for several Ru chromophores were higher than those for well-known inorganic crystals. With decreasing temperature, the SHG signal strongly increases below 55 K and correlates well with occurrence of "softlike" low-frequency anharmonic quasiphonon modes responsible for the phase transitions. The SHG maxima were observed at acoustic frequencies of about 13 kHz. Increasing of acoustical frequencies up to the megahertz range suppresses the observed phenomena. Comparing the obtained results with the acoustically induced Raman spectra at different temperatures one can conclude that the observed effects are due to acoustically induced electron-vibration anharmonicity, and are observed at temperatures below 55 K. Varying the chromophore content within the embedded matrices we were able to use effective nanoparticle sizes within the range 5-60 nm. It is clearly shown that the enhancement of the effective nanosize effectively suppresses the observed second-order optical effects.
  • χ<sup>(2)</sup> Grating in Ru Derivative Chromophores Incorporated within the PMMA Polymer Matrices
    作者:A. Migalska-Zalas、Z. Sofiani、B. Sahraoui、I. V. Kityk、S. Tkaczyk、V. Yuvshenko、J.-L. Fillaut、J. Perruchon、T. J. J. Muller
    DOI:10.1021/jp048794h
    日期:2004.9.1
    We have found that Ru derivative chromophores incorporated into the PMMA polymer matrices might be considered as promising materials for optical poling. The maximally achieved effective second-order optical susceptibility for the wavelength 1.89 mum is about 1.94 pm/V. The investigated composites possess metastable trapping levels originating both from the d states of Ru and due to effective charge transfer due to the presence of pi-conjugated states. Because of incorporation of the chromophore into polymer matrices, we have revealed that the maximal susceptibility is observed at 5-6% of the chromophore in weighting units. The further increase of the second-order susceptibility is limited by the appearance of chromophore agglomerates substantially restraining second-order susceptibilities. The investigated composites possess long-lived chi((2)) grating, which decreases less than 76% after 600 min of laser treatment. The electrostatic field causes additional reanimation of the second harmonic generation during the decay regime. The electron microscopy pictures clearly confirm appearance of the chi((2)) grating.
  • Design and Synthesis of Ruthenium Oligothienylacetylide Complexes. New Materials for Acoustically Induced Nonlinear Optics
    作者:Jean-Luc Fillaut、Johann Perruchon、Philippe Blanchard、Jean Roncali、Stéphane Golhen、Magali Allain、Anna Migalsaka-Zalas、Ivan V. Kityk、Bouchta Sahraoui
    DOI:10.1021/om049236s
    日期:2005.2.1
    A series of new donor−π-acceptor ruthenium acetylide systems built around thiophene-based π-conjugating spacers of different lengths have been developed. Comparison of the linear and third-order nonlinear optical properties of these donor−π-acceptor chromophores shows that the elongation of the oligothiophene-based spacer or further introduction of a double bond leading to a dithienylethylene spacer
    已经开发了一系列围绕不同长度的基于噻吩的π共轭间隔基构建的新的供体-π-受体钌钌系统。这些供体-π-受体生色团的线性和三阶非线性光学性质的比较表明,基于低聚噻吩的间隔基的延伸或进一步引入双键导致二噻吩基乙烯间隔基产生最大吸收的显着红移以及分子立方超极化性的显着增强。此外,对于掺入PMMA基质中的这些复合物的薄膜复合材料,还观察到了声诱发的第二谐波产生(AISHG),其值达到了迄今为​​止报道的最高值。
查看更多

同类化合物

试剂2,2'-Thieno[3,2-b]thiophene-2,5-diylbis-3-thiophenecarboxylicacid 苯并[b]噻吩,3-(2-噻嗯基)- 甲基[2,3'-联噻吩]-5-羧酸甲酯 牛蒡子醇 B 十四氟-Alpha-六噻吩 三丁基(5''-己基-[2,2':5',2''-三联噻吩]-5-基)锡 α-四联噻吩 α-六噻吩 α-五联噻吩 α-七噻吩 α,ω-二己基四噻吩 5,5′-双(3-己基-2-噻吩基)-2,2′-联噻吩 α,ω-二己基六联噻吩 Α-八噻吩 alpha-三联噻吩甲醇 alpha-三联噻吩 [3,3-Bi噻吩]-2,2-二羧醛 [2,2’]-双噻吩-5,5‘-二甲醛 [2,2':5',2''-三联噻吩]-5,5''-二基双[三甲基硅烷] [2,2'-联噻吩]-5-甲醇,5'-(1-丙炔-1-基)- [2,2'-联噻吩]-5-甲酸甲酯 [2,2'-联噻吩]-5-乙酸,a-羟基-5'-(1-炔丙基)-(9CI) C-[2,2-二硫代苯-5-基甲基]胺 5’-己基-2,2’-联噻吩-5-硼酸频哪醇酯 5-辛基-1,3-二(噻吩-2-基)-4H-噻吩并[3,4-c]吡咯-4,6(5H)-二酮 5-苯基-2,2'-联噻吩 5-溴5'-辛基-2,2'-联噻吩 5-溴-5′-己基-2,2′-联噻吩 5-溴-5'-甲酰基-2,2':5'2'-三噻吩 5-溴-3,3'-二己基-2,2'-联噻吩 5-溴-3'-癸基-2,2':5',2''-三联噻吩 5-溴-2,2-双噻吩 5-溴-2,2'-联噻吩-5'-甲醛 5-氯-5'-苯基-2,2'-联噻吩 5-氯-2,2'-联噻吩 5-正辛基-2,2'-并噻吩 5-己基-5'-乙烯基-2,2'-联噻吩 5-己基-2,2-二噻吩 5-全氟己基-5'-溴-2,2'-二噻吩 5-全氟己基-2,2′-联噻吩 5-乙酰基-2,2-噻吩基 5-乙氧基-2,2'-联噻吩 5-丙酰基-2,2-二噻吩 5-{[[2,2'-联噻吩]-5-基}噻吩-2-腈 5-[5-(5-己基噻吩-2-基)噻吩-2-基]噻吩-2-羧酸 5-(羟甲基)-[2,2]-联噻吩 5-(噻吩-2-基)噻吩-2-甲腈 5-(5-甲酰基-3-己基噻吩-2-基)-4-己基噻吩-2-甲醛 5-(5-甲基噻吩-2-基)噻吩-2-甲醛 5-(5-噻吩-2-基噻吩-2-基)噻吩-2-羧酸 5-(5-乙炔基噻吩-2-基)噻吩-2-甲醛