原子层沉积制备氧化锆、半氧化锆和氧化锆(HZO)超薄膜的铁电性和结晶度

Tzu-Yao Hsu, B. Lin, J. Shieh, Miin-Jang Chen
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摘要

通过热原子层沉积或远程等离子体原子层沉积(RP-ALD)制备了厚度在5 ~ 12 nm之间的氧化锆(HZO)固溶体超薄膜(包括纯氧化锆(ZrO2)和氧化锆(HfO2))和氧化锆/HfO2双层超薄膜。由于在RP-ALD过程中薄膜经历了等离子体诱导的热应力,具有高压正交(o)空间群Pbc21的ZrO2超薄膜可以在不退火的情况下实现铁电结晶。相比之下,对于ZrO2/HfO2双层超薄膜,由于HfO2的结晶温度较高,需要经过退火才能使夹在中间的HfO2层被ZrO2顶层和Si底层衬底充分约束,从而促进HfO2中高压铁电o相的形成。RP-ALD制备的HZO超薄膜的铁电性能高度依赖于hf - zr比,HfO2的增加对铁电性能不利,这主要是由于HfO2的高结晶温度。在未退火的情况下,HZO超薄膜的铁电性受等离子体处理诱导的非晶相和铁电性o相的相对数量控制。退火后,铁电性受铁电o相和非铁电单斜相(m)的相对数量控制。
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The Ferroelectricity and Crystallinity of Zirconia, Hafnia and Hafnium Zirconium Oxide (HZO) Ultrathin Films Prepared by Atomic Layer Deposition With and Without Post-Annealing
Large stable ferroelectricity in hafnium zirconium oxide (HZO) solid solution ultrathin films (including pure zirconia (ZrO2) and hafnia (HfO2)) and ZrO2/HfO2 bilayer ultrathin films of thickness ranging from 5–12 nm, prepared by thermal atomic layer deposition or remote plasma atomic layer deposition (RP-ALD) has been demonstrated. Ferroelectric crystallization of the ZrO2 ultrathin film with high-pressure orthorhombic (o) space group Pbc21 could be achieved without post-annealing due to the plasma-induced thermal stresses experienced by the film during the RP-ALD process. In contrast, for the ZrO2/HfO2 bilayer ultrathin film, due to the high crystallization temperature of HfO2, post-annealing was needed to achieve sufficient confinement of the sandwiched HfO2 layer by the ZrO2 top layer and Si bottom substrate to promote the high-pressure ferroelectric o-phase in HfO2. The ferroelectric properties of the HZO ultrathin films prepared by RP-ALD were highly dependent on the Hf-to-Zr ratio — an increasing amount of HfO2 has been found to be detrimental to the ferroelectricity, mainly due to the high crystallization temperature of HfO2. Without post-annealing, the ferroelectricity of the HZO ultrathin films was governed by the relative amounts of the amorphous phase and the ferroelectric o-phase induced by the plasma treatment. While with post-annealing, the ferroelectricity was governed by the relative amounts of the ferroelectric o-phase and the non-ferroelectric monoclinic (m) phase.
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