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首页> 外文期刊>Journal of Electronic Materials >Ti-Rich Barrier Layers Self-Formed on Porous Low-k Layers Using Cu(1 at.percent Ti) Alloy Films
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Ti-Rich Barrier Layers Self-Formed on Porous Low-k Layers Using Cu(1 at.percent Ti) Alloy Films

机译:使用Cu(1 at。%Ti)合金膜在多孔低k层上自形成的Ti富垒层

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摘要

To investigate the applicability of the technique of barrier self-formation using Cu(Ti) alloy films on porous low-k dielectric layers, Cu(1 at.percent Ti) alloy films were deposited on porous SiOCH (low-k) dielectric layers in samples with and without approx6.5-nm-thick SiCN pore seals. Ti-rich barrier layers successfully self-formed on the porous low-k layer of both sample types after annealing in Ar for 2 h at 400 deg C to 600 deg C. The Ti-rich barrier layers consisted of amorphous Ti oxides and polycrystalline TiC for the samples without pore sealing, and amorphous TiN, TiC, and Ti oxides for the pore-sealed samples. The amorphous TiN originated from reaction of Ti atoms with the pore seal, and formed beneath the Cu alloy films. This may explain two peaks of Ti segregation at the interface that appeared in Rutherford backscattering spectroscopy (RBS) profiles, and suggests that the Ti-rich barrier layers self-formed by the reaction of Ti atoms with the pore seal and porous low-k layers separately. The total molar amount of Ti atoms segregated at the interface in the pore-sealed samples was larger than that in the samples without pore sealing, resulting in lower resistivity. On the other hand, resistivity of the Cu alloy films annealed on the porous low-k layers was lower than that annealed on the nonporous low-k layers. Coarser Cu columnar grains were observed in the Cu alloy films annealed on the porous low-k layers, although the molar amount of Ti atoms segregated at the interface was similar in both sample types after annealing. The cause could be faster reaction of the Ti atoms with the porous dielectric layers.
机译:为了研究在多孔低k介电层上使用Cu(Ti)合金膜进行势垒自形成技术的适用性,将Cu(1 at。%Ti)合金膜沉积在多孔SiOCH(低k)介电层中。具有和不具有约6.5 nm厚的SiCN孔密封的样品。富钛的阻挡层在两种样品类型的多孔低介电常数k层中在400摄氏度至600摄氏度的Ar中退火2小时后成功地自形成。富钛的阻挡层由非晶态Ti氧化物和多晶TiC组成对于没有孔密封的样品,无定形TiN,TiC和Ti氧化物用于孔密封的样品。非晶态TiN源自Ti原子与孔隙密封的反应,并在Cu合金膜下形成。这可能解释了在卢瑟福背散射光谱(RBS)轮廓中出现的界面处的Ti偏析的两个峰,并表明富含Ti的势垒层是通过Ti原子与孔隙密封和多孔低k层反应而自形成的分别。与未进行气孔密封的样品相比,在气孔密封样品的界面处偏析的Ti原子的总摩尔量大,导致电阻率降低。另一方面,在多孔低k层上退火的Cu合金膜的电阻率比在无孔低k层上退火的电阻率低。在退火后的两种样品中,虽然在两种低合金层上退火的Cu合金膜中均观察到了粗大的Cu柱状晶粒,但在界面处偏析的Ti原子的摩尔量相似。原因可能是Ti原子与多孔介电层的反应更快。

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