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arXiv 2008.13709cond-mat.mtrl-sci
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含能离子在HiPIMS沉积Ti膜中fcc和ω晶相生长中的作用

Role of energetic ions in the growth of fcc and ω crystalline phases in Ti films deposited by HiPIMS

David Dellasega, Francesco Mirani, Davide Vavassori, Claudia Conti, Matteo Passoni

摘要:

钛(Ti)由于其优异的性能而被广泛应用于薄膜技术中,通常导致制备α相(hcp)Ti膜。在这项工作中,我们研究了不同类型和能量的成膜物种沉积的Ti膜的相演变。为了研究不同的等离子体物种环境,通过使用常规的直流磁控溅射(DCMS)和高功率脉冲磁控溅射(HiPIMS)生长具有不同厚度的膜。此外,HiPIMS沉积与不同的衬底偏置电压US(0 V,-300 V和-500 V)进行调查不同的离子能量范围。微结构,形貌和残余应力的沉积膜,以及DCMS和HiPIMS等离子体组成,分析与不同的表征技术。DCMS样品仅显示Ti α相,并且显示拉伸残余应力随厚度减小。就HiPIMS样品而言,随着厚度增加,观察到残余应力的压缩-拉伸-压缩(CTC)行为。具体地,在低能量离子条件(US =0 V)下沉积的膜显示出最大厚度为约370 nm的Ti fcc相的存在。随后,在高能量条件(US = -300 V和-500 V)下沉积的膜分别显示厚度大于260和330 nm的Ti ω-相的成核。考虑到不同的沉积条件,这些不寻常的Ti相的形成进行了讨论。

英文摘要:

Titanium (Ti), due to its excellent properties, is widely exploited in thin film technology that usually leads to the production of α-phase (hcp) Ti films. In this work, we investigate the phase evolution of Ti films deposited by varying type and energy of the film-forming species. To investigate different plasma species environments, films with different thicknesses are grown by using conventional Direct Current Magnetron Sputtering (DCMS) and High Power Impulse Magnetron Sputtering (HiPIMS). Furthermore, HiPIMS depositions with different substrate bias voltage US (0 V, -300 V and -500 V) are performed to investigate different ion energy ranges. Microstructure, morphology and residual stress of the deposited films, as well as the DCMS and HiPIMS plasma composition, are analysed with different characterization techniques. The DCMS samples exhibit the Ti α-phase only and show a tensile residual stress decreasing with thickness. As far as HiPIMS samples are concerned, a compressive-tensile-compressive (CTC) behavior is observed for residual stresses as thickness increases. Specifically, films deposited in low energy ion conditions (US =0 V) show the presence of the Ti fcc phase up to a maximum thickness of about 370 nm. Differently, films deposited under high energy conditions (US = -300 V and -500 V) show the nucleation of the Ti ω-phase for thicknesses greater than 260 and 330 nm, respectively. The formation of these unusual Ti phases is discussed considering the different deposition conditions.

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