Truscott Benjamin S, Kelly Mark W, Potter Katie J, Ashfold Michael N R, Mankelevich Yuri A
School of Chemistry, University of Bristol , Bristol BS8 1TS, U.K.
Skobel'tsyn Institute of Nuclear Physics, Moscow State University , Leninskie gory, Moscow 119991, Russia.
J Phys Chem A. 2016 Nov 3;120(43):8537-8549. doi: 10.1021/acs.jpca.6b09009. Epub 2016 Oct 24.
We report a combined experimental and modeling study of microwave-activated dilute CH/N/H plasmas, as used for chemical vapor deposition (CVD) of diamond, under very similar conditions to previous studies of CH/H, CH/H/Ar, and N/H gas mixtures. Using cavity ring-down spectroscopy, absolute column densities of CH(X, v = 0), CN(X, v = 0), and NH(X, v = 0) radicals in the hot plasma have been determined as functions of height, z, source gas mixing ratio, total gas pressure, p, and input power, P. Optical emission spectroscopy has been used to investigate, with respect to the same variables, the relative number densities of electronically excited species, namely, H atoms, CH, C, CN, and NH radicals and triplet N molecules. The measurements have been reproduced and rationalized from first-principles by 2-D (r, z) coupled kinetic and transport modeling, and comparison between experiment and simulation has afforded a detailed understanding of C/N/H plasma-chemical reactivity and variations with process conditions and with location within the reactor. The experimentally validated simulations have been extended to much lower N input fractions and higher microwave powers than were probed experimentally, providing predictions for the gas-phase chemistry adjacent to the diamond surface and its variation across a wide range of conditions employed in practical diamond-growing CVD processes. The strongly bound N molecule is very resistant to dissociation at the input MW powers and pressures prevailing in typical diamond CVD reactors, but its chemical reactivity is boosted through energy pooling in its lowest-lying (metastable) triplet state and subsequent reactions with H atoms. For a CH input mole fraction of 4%, with N present at 1-6000 ppm, at pressure p = 150 Torr, and with applied microwave power P = 1.5 kW, the near-substrate gas-phase N atom concentration, [N], scales linearly with the N input mole fraction and exceeds the concentrations [NH], [NH], and [CN] of other reactive nitrogen-containing species by up to an order of magnitude. The ratio [N]/[CH] scales proportionally with (but is 10-10 times smaller than) the ratio of the N to CH input mole fractions for the given values of p and P, but [N]/[CN] decreases (and thus the potential importance of CN in contributing to N-doped diamond growth increases) as p and P increase. Possible insights regarding the well-documented effects of trace N additions on the growth rates and morphologies of diamond films formed by CVD using MW-activated CH/H gas mixtures are briefly considered.
我们报告了一项关于微波激活的稀CH/N/H等离子体的实验与建模相结合的研究,该等离子体用于金刚石的化学气相沉积(CVD),实验条件与先前对CH/H、CH/H/Ar和N/H气体混合物的研究非常相似。利用光腔衰荡光谱技术,已测定了热等离子体中CH(X, v = 0)、CN(X, v = 0)和NH(X, v = 0)自由基的绝对柱密度随高度z、源气体混合比、总气压p和输入功率P的变化关系。利用发射光谱技术,针对相同变量研究了电子激发态物种的相对数密度,即H原子、CH、C、CN和NH自由基以及三重态N分子。通过二维(r, z)耦合动力学和输运模型从第一性原理对测量结果进行了再现和合理化分析,实验与模拟之间的比较使我们对C/N/H等离子体化学反应性以及随工艺条件和反应器内位置的变化有了详细的了解。经过实验验证的模拟已扩展到比实验探测的更低的N输入分数和更高的微波功率,为金刚石表面附近的气相化学及其在实际金刚石生长CVD工艺中广泛使用的各种条件下的变化提供了预测。在典型的金刚石CVD反应器中普遍存在的输入微波功率和压力下,强束缚的N分子非常抗解离,但其化学反应性通过在其最低(亚稳态)三重态中的能量汇聚以及随后与H原子的反应而增强。对于CH输入摩尔分数为4%,N含量为1 - 6000 ppm,压力p = 150 Torr,施加微波功率P = 1.5 kW的情况,近衬底气相N原子浓度[N]与N输入摩尔分数呈线性关系,并且比其他含活性氮物种的浓度[NH]、[NH]和[CN]高出一个数量级。对于给定的p和P值,[N]/[CH]与N和CH输入摩尔分数的比值成比例(但比其小10 - 10倍),但随着p和P的增加,[N]/[CN]降低(因此CN对N掺杂金刚石生长的潜在重要性增加)。简要考虑了关于微量N添加对使用微波激活的CH/H气体混合物通过CVD形成的金刚石薄膜的生长速率和形貌的文献记载效应的可能见解。