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Effects in Surface Free Energy of Sputter-Deposited VN_x Films

机译:溅射沉积的VN_x薄膜表面自由能的影响

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摘要

Vanadium nitride (VN_x) thin films have attracted much attention for semiconductor integrated circuit (IC) packaging molding dies, and forming tools due to their excellent hardness and, thermal stability. VN_x thin films with VN0.45, VN_(0.83), VN_(1.22), VN_(1.73), VN_(2.06) were prepared using a radio frequency (RF) sputter technique. The experimental results showed that the contact angle at 20° C increases with increasing nitrogen content of the VN_x films, to 101.4° corresponding to VN_(1.73) and then decreased. In addition, the contact angles decreased with increasing surface temperature, because an increase of the surface temperature disrupts the hydrogen bonds between water and the films and the water gradually vaporizes. The total surface fee energy (SFE) at 20°C decreased with nitrogen content of the VN_x films to 29.8 mN/m (VN_(1.73)) and then increased. This is because a larger contact angle means weaker hydrogen bonding which results in a lower SFE. The polar SFE component had the same trend as the total SFE, but the dispersive SFE component had the opposite trend. The polar SFE component is also lower than the dispersive SFE component. This is because hydrogen bonds are polar. The total SFE, dispersive SFE and polar SFE of the VN_x films all decrease with increasing surface temperature. This is because with increasing temperature, water evaporates from the surface, disrupting hydrogen bonds and hence increasing surface entropy. The film roughness has an obvious effect on the SFE and there is tendency for the SFE to increase with increasing film surface roughness. As a result the SFE and surface roughness can be expressed in terms of a simple ratio function.
机译:氮化钒(VN_x)薄膜因其优异的硬度和热稳定性而备受半导体集成电路(IC)封装成型模具和成型工具的关注。使用射频(RF)溅射技术制备具有VN0.45,VN_(0.83),VN_(1.22),VN_(1.73),VN_(2.06)的VN_x薄膜。实验结果表明,随着VN_x膜中氮含量的增加,在20°C时的接触角增大,对应于VN_(1.73)增大到101.4°,然后减小。另外,接触角随着表面温度的升高而减小,这是因为表面温度的升高破坏了水与膜之间的氢键,并且水逐渐蒸发。随着VN_x膜中氮含量的降低,20°C时的总表面能(SFE)降低至29.8 mN / m(VN_(1.73)),然后增加。这是因为较大的接触角意味着较弱的氢键结合,从而导致较低的SFE。极性SFE成分的趋势与总SFE成分的趋势相同,但分散SFE成分的趋势相反。极性SFE组分也低于分散SFE组分。这是因为氢键是极性的。 VN_x薄膜的总SFE,分散SFE和极性SFE都随着表面温度的升高而降低。这是因为随着温度的升高,水从表面蒸发,破坏了氢键,从而增加了表面的熵。膜粗糙度对SFE有明显的影响,并且SFE有随着膜表面粗糙度增加而增加的趋势。结果,可以用简单的比率函数表示SFE和表面粗糙度。

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