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通过后热处理控制晶格应变以制备无裂纹且坚固的铁电钛酸钡薄膜。

Controlling of lattice strains for crack-free and strong ferroelectric barium titanate films by post-thermal treatment.

作者信息

Kim Bogyu, Jeon Young-Uk, Lee Chulwoo, Kim In Soo, Lee Byeong-Hyeon, Kim Young-Hwan, Kim Young Duck, Han Il Ki, Lee Kwanil, Kim Jongbum, Kang JoonHyun

机构信息

Nanophotonics Research Center, Korea Institute of Science and Technology (KIST), Seoul, 02792, Republic of Korea.

KHU-KIST Department of Converging Science and Technology, Kyung Hee University, Seoul, 02447, Republic of Korea.

出版信息

Sci Rep. 2022 Mar 30;12(1):5363. doi: 10.1038/s41598-022-09182-0.

DOI:10.1038/s41598-022-09182-0
PMID:35354865
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC8967881/
Abstract

In this study, we experimentally demonstrate fabrication of ultra-smooth and crystalline barium titanate (BTO) films on magnesium oxide (MgO) substrates by engineering lattice strain and crystal structure via thermal treatment. We observe that oxygen-depleted deposition allows growth of highly strained BTO films on MgO substrates with crack-free surface. In addition, post-thermal treatment relaxes strain, resulting in an enhancement of ferroelectricity. Surface roughening of the BTO films caused by recrystallization during post-thermal treatment is controlled by chemical-mechanical polishing (CMP) to retain their initial ultra-smooth surfaces. From Raman spectroscopy, reciprocal space map (RSM), and capacitance-voltage (C-V) curve measurements, we confirm that the ferroelectricity of BTO films strongly depend on the relaxation of lattice strain and the phase transition from a-axis to c-axis oriented crystal structure.

摘要

在本研究中,我们通过热处理工程晶格应变和晶体结构,实验证明了在氧化镁(MgO)衬底上制备超光滑且结晶的钛酸钡(BTO)薄膜。我们观察到,贫氧沉积允许在MgO衬底上生长具有无裂纹表面的高应变BTO薄膜。此外,后热处理可松弛应变,从而增强铁电性。通过化学机械抛光(CMP)控制后热处理过程中再结晶引起的BTO薄膜表面粗糙度,以保持其初始超光滑表面。通过拉曼光谱、倒易空间映射(RSM)和电容-电压(C-V)曲线测量,我们证实BTO薄膜的铁电性强烈依赖于晶格应变的松弛以及从a轴到c轴取向晶体结构的相变。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b833/8967881/9020ccc0c5c1/41598_2022_9182_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b833/8967881/9494dd59cfe9/41598_2022_9182_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b833/8967881/0a302efc4f65/41598_2022_9182_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b833/8967881/8c420ecf0f4f/41598_2022_9182_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b833/8967881/5cb1c3515247/41598_2022_9182_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b833/8967881/9020ccc0c5c1/41598_2022_9182_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b833/8967881/9494dd59cfe9/41598_2022_9182_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b833/8967881/0a302efc4f65/41598_2022_9182_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b833/8967881/8c420ecf0f4f/41598_2022_9182_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b833/8967881/5cb1c3515247/41598_2022_9182_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b833/8967881/9020ccc0c5c1/41598_2022_9182_Fig5_HTML.jpg

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