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Synthesis of cubic boron nitride thin films by microwave PECVD

机译:微波PECVD法合成立方氮化硼薄膜

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Boron nitride can be synthesised in two major crystalline polytypes, the hexagonal (h-BN) and the cubic one (c-BN), related respectively to the sp2 and the sp3 hybridation of the chemical bondings of both atomic species. The cubic form is very attractive, due to its extreme properties, similar to those of diamond in term of hardness, thermal conductivity, chemical inertness and optical transparency, It is even more stable against oxidation up to higher temperature, and can be doped whether P or N type, making it a candidate for applications in power electronics. Classically, c-BN can be synthesised under high pressure and high temperature, but more recently PVD and CVD have been successfully employed to obtain thin films. In these later cases, the growth process requires bombardment with energetic particles, and general ways the structure is left in compressive stress after deposition and delamination or cracking of the film can occur. We have deposited boron nitride thin films on silicon substrates at low temperature (below 300/spl deg/C) in a microwave plasma enhanced chemical vapor deposition (PECVD) apparatus, An organometallic compound, borane dimethyl amine, was used as boron precursor. To promote the growth of the cubic phase a negative self bias was applied to the sample holder by mean of a 13.56 MHz RF signal. Characterisation of the samples involve infra red and Raman spectrometries, and atomic force microscopy. Films containing a fraction of c-BN, as high as 98%, have been obtained, as can be seen on the infra red spectra. The ratio has been determined according to the relative intensity of the active IR mode of the cubic and the hexagonal phases. At normal incidence only the transversal optical (TO) modes are observed, whereas at oblique incidence the longitudinal optical (LO) modes are also evidenced, according to the Berreman effect. The c-BN TO absorption band is observed at 1071 cm/sup -1/ and its associated LO mode is located at 1267 cm/sup -1/. The films exhibit a very low roughness, as observe by atomic force microscopy, and contain nanocrystals of about 10 nm averaged size, as deduced from the Raman measurements. These deposits are very adherent and do not delaminate even after more than one year. Also, PECVD seems to be a promising method for the synthesis of c-BN layers.
机译:氮化硼可以合成为两种主要的晶体多型,六方型(h-BN)和立方型(c-BN),分别与两个原子种类的化学键的sp2和sp3杂化有关。立方晶由于其极好的特性而非常吸引人,在硬度,导热性,化学惰性和光学透明性方面与金刚石相似,在高温下甚至更稳定地抗氧化,并且是否可以掺杂P或N型,使其成为电力电子应用的候选者。经典地,可以在高压和高温下合成c-BN,但是近来PVD和CVD已经成功地用于获得薄膜。在这些较后的情况下,生长过程需要用高能粒子轰击,并且在薄膜沉积,分层或破裂后,结构通常处于压缩应力状态。我们已经在微波等离子增强化学气相沉积(PECVD)装置中在低温(低于300 / spl deg / C)下在硅基板上沉积了氮化硼薄膜,有机金属化合物硼烷二甲基胺被用作硼前驱物。为了促进立方相的生长,通过13.56 MHz的RF信号对样品架施加了负自偏压。样品的表征涉及红外和拉曼光谱,以及原子力显微镜。如在红外光谱上所见,已经获得了含有高达98%的c-BN的膜。该比例是根据立方相和六方相的有源红外模式的相对强度确定的。根据Berreman效应,在法向入射时仅观察到横向光学(TO)模式,而在斜入射时还观察到纵向光学(LO)模式。在1071 cm / sup -1 /处观察到c-BN TO吸收带,其相关的LO模式位于1267 cm / sup -1 /。如通过原子力显微镜所观察到的,膜表现出非常低的粗糙度,并且包含由拉曼测量得出的平均尺寸为约10nm的纳米晶体。这些沉积物具有很强的附着力,即使超过一年也不会分层。而且,PECVD似乎是用于合成c-BN层的有前途的方法。

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