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SIGMA 358746-1G 四十四烷 7098-22-8

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  • ¥1993
  • Sigma-Aldrich
  • 进口
  • 358746-1G
  • 2025年08月13日
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    • 详细信息
    • 文献和实验
    • 技术资料
    • 保存条件

      常温

    • 保质期

      根据瓶身LOT号查询

    • 英文名

      Tetratetracontane

    • 库存

      有现货

    • 供应商

      浙江羽翔生物科技有限公司

    • CAS号

      7098-22-8

    • 规格

      1G

    属性

    质量水平

    200

    方案

    99%

    mp

    85-87 °C (lit.)

    SMILES字符串

    CCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCCC

    InChI

    1S/C44H90/c1-3-5-7-9-11-13-15-17-19-21-23-25-27-29-31-33-35-37-39-41-43-44-42-40-38-36-34-32-30-28-26-24-22-20-18-16-14-12-10-8-6-4-2/h3-44H2,1-2H3

    InChI key

    KMXFZRSJMDYPPG-UHFFFAOYSA-N

    一般描述

    四十四烷是一种长链烷烃。它是巨枝大戟(Euphorbia macroclada)精油的主要成分。 四十四烷与[Na(H2O)P5W30O110] 的共吸附会在四十四烷的缓冲层上形成单个分离的表面活性剂包封簇,这是通过扫描隧道显微术确定的。 已经报道了四十四烷的热氧化降解反应。

    应用

    为了提高电荷载流子迁移率,可以在铜-酞菁场效应晶体管的钝化层中使用四十四烷。它可用于修饰Au(111)上的准二维表面电子系统,已通过角分辨光电子能谱法对其进行了研究。

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    图标文献和实验
    该产品被引用文献

    Images of paraffin monolayer crystals with perfect contrast: minimization of beam-induced specimen motion.

    Ultramicroscopy (2010-12-28)
    R M Glaeser, G McMullan, A R Faruqi, R Henderson
    PMID21185452
    摘要

    Quantitative analysis of electron microscope images of organic and biological two-dimensional crystals has previously shown that the absolute contrast reached only a fraction of that expected theoretically from the electron diffraction amplitudes. The accepted explanation for this is that irradiation of the specimen causes beam-induced charging or movement, which in turn causes blurring of the image due to image or specimen movement. In this paper, we used three different approaches to try to overcome this image-blurring problem in monolayer crystals of paraffin. Our first approach was to use an extreme form of spotscan imaging, in which a single image was assembled on film by the successive illumination of up to 50,000 spots, each of a diameter of around 7 nm. The second approach was to use the Medipix II detector with its zero-noise readout to assemble a time-sliced series of images of the same area in which each frame from a movie with up to 400 frames had an exposure of only 500 electrons. In the third approach, we simply used a much thicker carbon support film to increase the physical strength and conductivity of the support. Surprisingly, the first two methods involving dose fractionation in space or time produced only partial improvements in contrast whereas the third approach produced many virtually perfect images, where the absolute contrast predicted from the electron diffraction amplitudes was observed in the images. We conclude that it is possible to obtain consistently almost perfect images of beam-sensitive specimens if they are attached to an appropriately strong and conductive support; however great care is needed in practice and the problem remains of how to best image ice-embedded biological structures in the absence of a strong, conductive support film.

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    SIGMA 358746-1G 四十四烷 7098-22-8
    ¥1993