Synthesis of cubic boron nitride thin films by microwave PECVD

P. Thévenin, A. Soltani, A. Bath
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Abstract

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.
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微波PECVD法制备立方氮化硼薄膜
氮化硼可以合成两种主要的晶体类型,六方(h-BN)和立方(c-BN),分别与两种原子的化学键的sp2和sp3杂化有关。立方形式是非常有吸引力的,由于其极端的性质,类似于那些金刚石在硬度,导热性,化学惰性和光学透明度方面,它是更稳定的抗氧化到更高的温度,并且可以掺杂无论是P或N型,使其成为候选应用于电力电子。传统上,c-BN可以在高压和高温下合成,但最近PVD和CVD已成功地用于制备薄膜。在这些后一种情况下,生长过程需要高能粒子轰击,一般情况下,沉积后结构处于压应力状态,薄膜可能发生分层或开裂。在微波等离子体增强化学气相沉积(PECVD)装置中,在低温(低于300/spl℃)下在硅衬底上沉积氮化硼薄膜,以有机金属化合物硼烷二甲基胺为硼前驱体。为了促进立方相的生长,在样品支架上施加了13.56 MHz射频信号的负自偏置。样品的表征包括红外光谱和拉曼光谱,以及原子力显微镜。从红外光谱上可以看出,已经得到了含有c-BN部分的薄膜,其含量高达98%。根据立方相和六边形相的有源红外模式的相对强度确定了该比值。根据Berreman效应,在正入射下只观察到横向光学(TO)模式,而在斜入射下也可以观察到纵向光学(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/处。通过原子力显微镜观察到,薄膜的粗糙度非常低,并且包含平均尺寸约为10纳米的纳米晶体,这是由拉曼测量得出的。这些沉积物非常粘着,即使在一年多后也不会分层。此外,PECVD似乎是一种很有前途的合成c-BN层的方法。
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