Direct Determination of Medium Range Ordering in Amorphous Hydrogenated Boron Carbide for Low-k Dielectric Applications
Direct Determination of Medium Range Ordering in Amorphous Hydrogenated Boron Carbide for Low-k Dielectric Applications
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直接测定低 k 电介质应用中非晶态氢化碳化硼的中程有序度
DOI:
10.1017/s143192762001394x
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发表时间:
2020
影响因子:
2.8
通讯作者:
Hwang, Jinwoo
中科院分区:
文献类型:
--
作者:
Gharacheh, Mehrdad Abbasi;Im, Soohyun;Johnson, Jared;Ortiz, Gabriel Calderon;Zhu, Menglin;Oyler, Nathan;Paquette, Michelle;Rulis, Paul;Sakidja, Ridwan;Hwang, Jinwoo
During past decades, the frequency of micro-processors has increased from 66MHz to 4 GHz while their sizes have decreased from 1 μm to 90 nm. As the size of interconnections (Fig. 1a) reduces, the conductors’ resistance and insulators’ capacitance increase, leading to increase in Resistance-Capacitance (RC) delay of ICs. It is important to decrease either conductors’ resistance or dielectrics’ capacitance to have more densely integrated transsitors and less RC delay [1]. To achieve this, there have been ongoing efforts to substitute traditional SiO2 with new generation of low dielectric constant (k) materials. Simultaneously, it is crucial to have stability in mechanical and thermal properties along with low dielectric constant [2-3].Amorphous hydrogenated boron carbide (a-BC: H) is a desired option containing both proper mechanical properties and low dielectric constant. The a-BC: H films can be grown using plasma enhanced chemical vapor deposition (PECVD) with ortho-carborane precursors [4], which results in a wide range of variation in the structure and composition. Theoretical modeling of amorphous hydrogenated boron carbide has suggested that atomic structure of a-BC: H contains 12-vertex icosahedral clusters which are attributed to short range ordering (SRO, Fig. 2b)[5]. These SRO clusters may gather and form the medium range ordering (MRO). However, it is currently not clear whether MRO information from these simulations is accurate since some simulation parameters (such as the time scale) are substantially different from the real growth conditions. The MRO parameters, if properly characterized, will provide us the opportunity to control the properties of the amorphous films by precisely controlling the PECVD growth conditions. However, MRO characterization has been challenging because conventional imaging or diffraction techniques tend to be insensitive to MRO.