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首页> 外文期刊>IEEE Transactions on Advanced Packaging >Effects in Surface Free Energy of Sputter-Deposited TaNx Films
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Effects in Surface Free Energy of Sputter-Deposited TaNx Films

机译:溅射沉积TaNx薄膜表面自由能的影响

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摘要

TaNx 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. Tantalum nitride (TaNx) thin films with TaN$_{0.63}$, TaN$_{1.14}$, TaN $_{1.58}$, TaN$_{2.19}$ , and TaN$_{2.81}$ were prepared using radio frequency (RF) sputter. The experimental results showed that the contact angle at 20 $^{circ}$ C go up with raising ${rm N}_{2}$ content to 119.2$^{circ}$ at beginning, corresponding to TaN $_{1.58}$, and then drop off. In addition, the contact angle components decreased with increasing surface temperature. Because increasing surface temperature disrupts the hydrogen bonds between water and the films and water vaporize gradually. The total surface free energy (SFE) at 20 $^{circ}$C decrease with ${rm N}_{2}$ content to raise to 39.6 mN/m(TaN$_{1.58}$) at the start, and then increase. A larger contact angle means a weaker hydrogen bonding, resulting in a lower SFE. The polar SFE component has same trend with total SFE, but the dispersive SFE component is on the contrary exactly. The polar SFE component is also lower than the dispersive SFE component. This results from hydrogen bonding being polar. The total SFE, dispersive SFE, and polar SFE of TaNx films decreased with increasing surface temperature. This is because water evaporation on the surface, disrupted hydrogen bonds, and surface entropy increase with increasing temperature. The film roughness has an obvious effect on the SFE and there is a tendency for the SFE to increase with increasing film surface roughness. SFE and surface roughness can be expressed as a function in direct ratio.
机译:TaNx薄膜具有出色的硬度和热稳定性,因此已引起半导体集成电路(IC)封装成型模具和成型工具的广泛关注。制备具有TaN $ _ {{0.63} $,TaN $ _ {1.14} $,TaN $ _ {1.58} $,TaN $ _ {2.19} $和TaN $ _ {2.81} $的氮化钽(TaNx)薄膜使用射频(RF)溅射。实验结果表明,接触角在20°C时开始增加$ {rm N} _ {2} $含量至119.2 $ ^ {circ} $,相当于TaN $ _ {1.58 } $,然后下车。另外,接触角分量随着表面温度的升高而降低。由于升高的表面温度破坏了水和薄膜之间的氢键,水逐渐蒸发。开始时,总表面自由能(SFE)在20 $ ^ {circ} $ C时降低,其中$ {rm N} _ {2} $的含量在开始时提高到39.6 mN / m(TaN $ _ {1.58} $),然后增加。较大的接触角意味着较弱的氢键,导致较低的SFE。极性SFE分量与总SFE趋势相同,但分散SFE分量恰恰相反。极性SFE组分也低于分散SFE组分。这是由于氢键是极性的。 TaNx薄膜的总SFE,分散SFE和极性SFE随着表面温度的升高而降低。这是因为表面上的水蒸发,氢键断裂和表面熵随温度升高而增加。膜粗糙度对SFE具有明显的影响,并且SFE有随着膜表面粗糙度增加而增加的趋势。 SFE和表面粗糙度可以直接比例表示。

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