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Atomic layer deposition of high-quality Pt thin film as an alternative interconnect replacing Cu
Journal of Vacuum Science & Technology A ( IF 2.9 ) Pub Date : 2020-03-19 , DOI: 10.1116/1.5134696
Seung-Min Han 1 , Dip K. Nandi 1 , Yong-Hwan Joo 1 , Toshiyuki Shigetomi 2 , Kazuharu Suzuki 2 , Shunichi Nabeya 2 , Ryosuke Harada 2 , Soo-Hyun Kim 1
Affiliation  

High-quality Pt thin films are prepared by atomic layer deposition (ALD) using metal-organic precursors dimethyl-(N,N-dimethyl-3-butene-1-amine-N) platinum (C8H19NPt) and with diluted molecular oxygen (O2) as a reactant. The films are grown at a relatively low temperature of 225 °C on a thermally grown SiO2 substrate, and the process shows all the necessary qualities of an ideal ALD such as self-limiting growth characteristics and a well-defined ALD temperature window between 200 and 250 °C. Noticeably, the current ALD-Pt process shows a very high growth per cycle of 0.167 nm without an incubation period at 225 °C, and perfect conformality is obtained at a dual trench structure (top and bottom width: 40 and 15 nm) with an aspect ratio of around 6.3. The resistivity of the ALD-Pt film at ∼39 nm in thickness deposited at 225 °C is almost the same (∼10.8 μΩ cm) as its bulk resistivity (10.6 μΩ cm), and it is as low as ∼12 μΩ cm at 25 nm in thickness. Comprehensive analyses using x-ray photoelectron spectroscopy, x-ray diffractometry, transmission electron microscopy (TEM), and x-ray reflectance indicate that the extremely low resistivity of ALD-Pt is due to the formation of highly pure and polycrystalline films with high density (∼21.04 g/cm3) and large grain size (∼48 nm for 25 nm thick film). For comparison, ALD-Ru is deposited at the same equipment and deposition temperature, 225 °C, using (ethylbenzene)(1,3-butadiene)Ru(0) (C12H16Ru) and diluted O2 as the reactant. The higher resistivity of ∼20 μΩ cm at a similar thickness (∼23.5 nm) with ALD-Pt is obtained, which is much higher than its bulk value (7.6 μΩ cm). TEM analysis suggests that the formation of relatively smaller-sized grains of ALD-Ru is the main reason for it.

中文翻译:

高质量Pt薄膜的原子层沉积作为替代Cu的替代互连

使用金属有机前体二甲基-(N,N-二甲基-3-丁烯-1-胺-N)铂(C 8 H 19 NPt)并通过稀释原子层沉积(ALD)制备高质量的Pt薄膜分子氧(O 2)作为反应物。薄膜在225°C的相对较低温度下在热生长的SiO 2上生长基板,并且该过程显示出理想ALD的所有必需质量,例如自限生长特性和200至250°C之间的ALD温度窗口。值得注意的是,当前的ALD-Pt工艺显示每周期0.167 nm的增长非常快,没有在225°C的潜伏期,并且在双沟槽结构(顶部和底部宽度:40和15 nm)下获得了完美的保形性。长宽比约为6.3。在ALD-Pt膜在厚度沉积在225℃~39处的电阻率几乎是相同的(~10.8  μ作为其体电阻率(Ω10.6厘米)  μ Ω厘米),并且它是低达〜12  μ厚度为25 nm时为Ωcm。使用X射线光电子能谱,X射线衍射法,透射电子显微镜(TEM)和X射线反射率进行的综合分析表明,ALD-Pt的极低电阻率是由于形成了高纯度的高密度多晶薄膜(〜21.04 g / cm 3)和大晶粒尺寸(对于25 nm厚的膜约为48 nm)。为了进行比较,使用(乙苯)(1,3-丁二烯)Ru(0)(C 12 H 16 Ru)和稀释的O 2作为反应物,在相同的设备和沉积温度225°C下沉积ALD-Ru 。约20的较高的电阻率 μ Ω厘米以类似的厚度(~23.5纳米)与ALD-Pt的获得,这是比其体积值高得多(7.6  μΩcm)。TEM分析表明,形成相对较小尺寸的ALD-Ru晶粒是主要原因。
更新日期:2020-03-19
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