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Optical properties of pyrolytic carbon deposits deduced from measurements of the extinction angle by polarized light microscopy

机译:通过偏振光显微镜测量消光角推导热解碳沉积物的光学特性

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摘要

The physical properties of graphite are considered a limit of the crystallization degree of pyrolytic carbon deposits. For instance, the spacing of basal planes of graphite is 0.335 nm while for pyrolytic carbon deposits it varies from 0.344 to 0.335 nm as annealing temperature increases 1. The ratio of pi- and sigma-bonding electronic states in graphite is 1/3, and the deviation from this value can be related to different texture degrees of pyrolytic carbon matrices of infiltrated carbon felts 2. On the contrary to other optical investigations 3 this correlation between graphite and pyrolytic carbon is not valid for polarized light microscopy, which is based on the optical anisotropy of pyrolytic carbon deposits and has been a benchmark for the rapid characterization of the texture degree of such materials for a long time. The measured extinction angles A_e for deposits usually exhibit values up to A_e approx=24 deg 4, which are significantly higher than the value of 16.3 deg reported for graphite 5 (Fig. 1). As graphite is considered the limit of the texture degree of pyrolytic carbon, the extinction angle of pyrolytic carbon is supposed to approach the value for graphite which is seemingly not the case.
机译:石墨的物理性质被认为是热解碳沉积物结晶程度的极限。例如,石墨基面的间距为0.335 nm,而对于热解碳沉积物,随着退火温度的升高,其间距从0.344 nm变化到0.335 nm[1]。石墨中π键和φ键电子态的比值为1/3,与该值的偏差可能与渗透碳毡的热解碳基质的不同织构程度有关[2]。与其他光学研究相反[3],石墨和热解碳之间的这种相关性不适用于偏振光显微镜,偏振光显微镜基于热解碳沉积物的光学各向异性,长期以来一直是快速表征此类材料织构程度的基准。矿床A_e测量的消光角通常高达A_e约=24度[4],明显高于石墨[5]报告的16.3度值(图1)。由于石墨被认为是热解碳质构度的极限,因此热解碳的消光角应该接近石墨的值,但事实似乎并非如此。

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