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首页> 外文期刊>The journal of physical chemistry, C. Nanomaterials and interfaces >Tetrahedral and Trigonal Carbon Atom Hybridization in Thin Amorphous Carbon Films Synthesized by Radio-Frequency Sputtering
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Tetrahedral and Trigonal Carbon Atom Hybridization in Thin Amorphous Carbon Films Synthesized by Radio-Frequency Sputtering

机译:射频溅射合成非晶碳薄膜中的四面体和三角碳原子杂化

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Ultrathin amorphous carbon (a-C) films were synthesized on Si(100) substrates by low-pressure, radio-frequency sputtering under different plasma discharge conditions. X-ray photoelectron spectroscopy (XPS) revealed different contents of C, Ar, Si, O, and N in the a-C films. The percentages of tetrahedral (sp~3) and trigonal (sp~2) carbon hybridizations in the films were determined from an analysis of the C1s core level spectra obtained by XPS narrow scanning. It is shown that the concentrations of surface chemisorbed O and N atoms from the ambient depend on the real surface area of the film (roughness effect). The binding energy shifts of the sp~2 and sp~3 hybridizations (observed after the decomposition of the C1s spectra) due to the Ar~+ ion bombardment are interpreted in terms of the residual compressive stress in the deposited a-C films. The mechanisms of sp~3 carbon hybridization are discussed in the context of XPS results. For negligible Ar~+ ion bombardment (zero substrate bias), sp~3 carbon hybridization is governed by a thermodynamic process that obeys the principle of minimum surface free energy. However, sp~3 carbon hybridization under plasma discharge conditions resulting in intense Ar~+ ion bombardment is controlled by collisions of Ar~+ ions with carbon atoms on the growing film surface and subsequent collisions between excited carbon atoms and other carbon atoms at the a-C film surface.
机译:通过在不同等离子放电条件下的低压射频溅射在Si(100)衬底上合成了超薄非晶碳(a-C)膜。 X射线光电子能谱(XPS)显示a-C膜中C,Ar,Si,O和N的含量不同。薄膜中四面体(sp〜3)和三角(sp〜2)碳杂化的百分比是通过对XPS窄扫描获得的C1s核心能级谱的分析来确定的。结果表明,从周围环境化学吸附的O和N原子的浓度取决于薄膜的实际表面积(粗糙度效应)。根据沉积的a-C膜中的残余压缩应力解释了由于Ar〜+离子轰击而引起的sp〜2和sp〜3杂交的结合能移动(在C1s光谱分解后观察到)。在XPS结果的背景下讨论了sp〜3碳杂交的机理。对于可忽略不计的Ar〜+离子轰击(零衬底偏压),sp〜3碳杂化由遵循最小表面自由能原理的热力学过程控制。然而,在等离子体放电条件下,sp〜3碳杂化导致强烈的Ar〜+离子轰击,受Ar〜+离子与生长膜表面上碳原子的碰撞以及随后在aC处激发的碳原子与其他碳原子之间的碰撞的控制薄膜表面。

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