Effect of Nitrogen Flow on the Growth of Nitrogen Ultrananocrystalline Diamond (N-UNCD) Films on Si/SiO2/HfO2 Substrate

Daniel Villarreal, F. Wittel, Anusha Rajan, Phillip Wittel, J. Alcantar-Peña, O. Auciello, E. Obaldía
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引用次数: 2

Abstract

This paper describes initial R&D focused on growing ultrananocrystalline diamond films (N-UNCD) with nitrogen (N) atoms incorporated in grain boundaries chemically reacted with C atoms dangling bonds and providing electrons for electrical conductivity. The N-UNCD films are grown on a thin layer of hafnium dioxide (HfO2), to explore the integration of N-UNCD films with the main gate oxide in current CMOS devices. The HfO2 template layer was grown by atomic layer deposition (ALD) on top of a 300 nm layer of silicon dioxide (SiO2) on a silicon substrate. The N-UNCD films are grown using the hot filament chemical vapor deposition (HFCVD) technique. A mixture of Ar/CH4/H2/N2 gases pass through an array of filaments heated to ~2300 °C to crack the CH4 and N2 molecules into C, CHx (x=1,2,3) and N atoms. The radicals react at the surface to grow the N-UNCD. The N-UNCD film density, morphology, and presence of N atoms, which induce electrical conductivity (resistivity), appears to depend mainly on the N2 flow, thus density of N atoms arrival to the substrate surface in conjunction with the film growth temperature. In previous work it was fond that a carbide layer is form beneath the UNCD for both Si, tungsten (W) and Hf. However, when N is added to the gas flow it reduces the coverage of UNCD over the HfO2 layer but not over the SiO2 layer. Large N2 flows (10-20 standard cubic cm, sccm) result in N-UNCD films with globular non-connected structures, resulting in high resistivities (several MW-cm to open circuit). X-ray Photoelectron Spectroscopy (XPS) analysis revealed the presence of both hafnium carbide (HfC) and hafnium nitride (HfxNy) on the surface of N-UNCD films grown on HfO2. The formation of HfxNy may compete with C for surface binding sites on the HfO2, inhibiting the formation of a HfC layer. There are several candidates of hafnium nitride (Hf3N2, Hf3N4. and HfN). Since the starting substrate material is hafnium(IV) oxide, and there is no oxygen flow during the N-UNCD film growth, the hypothesis is that, with large N2 flow (10-20 sccm), the formation of hafnium(IV) nitride is dominant. Hafnium(IV) nitride has an orthorhombic unit cell while hafnium (IV) carbide has a cubic unit cell structure, similar to diamond. Thus, the presence of Hf3N4 may inhibit diamond growth via a mismatch of unit cells at the interface. On the other hand, a low flow of N2 (6 sccm) combined with low flows of H and Ar, produced, good dense, very low resistivity N-UNCD films.
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氮流对Si/SiO2/HfO2衬底上氮超晶金刚石(N-UNCD)薄膜生长的影响
本文描述了最初的研发重点是在晶界中加入氮原子与C原子悬垂键发生化学反应并提供导电电子的超晶金刚石薄膜(N- uncd)的生长。N-UNCD薄膜生长在一层薄薄的二氧化铪(HfO2)上,以探索当前CMOS器件中N-UNCD薄膜与主栅氧化物的集成。采用原子层沉积法(ALD)在硅衬底上制备了一层300 nm的二氧化硅(SiO2)。采用热丝化学气相沉积(HFCVD)技术制备了N-UNCD薄膜。Ar/CH4/H2/N2混合气体通过加热至~2300℃的一系列细丝,将CH4和N2分子裂解为C、CHx (x=1,2,3)和N原子。自由基在表面反应生成N-UNCD。N- uncd薄膜的密度、形态和N原子的存在(它们会诱发电导率)似乎主要取决于N2流动,因此到达衬底表面的N原子密度与薄膜生长温度有关。在以前的工作中,人们倾向于在UNCD下形成硅、钨和铪的碳化物层。然而,当向气流中加入N时,它会减少UNCD在HfO2层上的覆盖,但不会减少在SiO2层上的覆盖。大的氮气流量(10-20标准立方厘米,sccm)会产生具有球状非连接结构的N-UNCD膜,从而产生高电阻率(开路时达到几毫微米)。x射线光电子能谱(XPS)分析表明,在HfO2上生长的N-UNCD薄膜表面同时存在碳化物铪(HfC)和氮化铪(HfxNy)。HfxNy的形成可能会与C竞争HfO2的表面结合位点,从而抑制HfC层的形成。有几种候选的氮化铪(Hf3N2, Hf3N4)。和HfN)。由于起始衬底材料为氧化铪,而在N-UNCD薄膜生长过程中没有氧气流动,因此假设在较大的N2流量(10-20 sccm)下,氮化铪的形成占主导地位。氮化铪具有正交晶胞结构,而碳化铪具有类似金刚石的立方晶胞结构。因此,Hf3N4的存在可能会通过界面上的单位细胞错配来抑制金刚石生长。另一方面,低流量的N2 (6 sccm)与低流量的H和Ar相结合,产生了致密、极低电阻率的N-UNCD薄膜。
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