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氧化铝添加对通过原子层沉积制备的二氧化钛薄膜和反蛋白石的光学性质及热稳定性的影响。

Influence of Alumina Addition on the Optical Properties and the Thermal Stability of Titania Thin Films and Inverse Opals Produced by Atomic Layer Deposition.

作者信息

Waleczek Martin, Dendooven Jolien, Dyachenko Pavel, Petrov Alexander Y, Eich Manfred, Blick Robert H, Detavernier Christophe, Nielsch Kornelius, Furlan Kaline P, Zierold Robert

机构信息

Institute of Nanostructure and Solid State Physics & Center for Hybrid Nanostructures, Universität Hamburg, Luruper Chausse 149, 22761 Hamburg, Germany.

Department of Solid State Sciences, COCOON Group, Ghent University, Krijgslaan 281/S1, B-9000 Ghent, Belgium.

出版信息

Nanomaterials (Basel). 2021 Apr 20;11(4):1053. doi: 10.3390/nano11041053.

DOI:10.3390/nano11041053
PMID:33924052
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC8074236/
Abstract

TiO thin films deposited by atomic layer deposition (ALD) at low temperatures (<100 °C) are, in general, amorphous and exhibit a smaller refractive index in comparison to their crystalline counterparts. Nonetheless, low-temperature ALD is needed when the substrates or templates are based on polymeric materials, as the deposition has to be performed below their glass transition or melting temperatures. This is the case for photonic crystals generated via ALD infiltration of self-assembled polystyrene templates. When heated up, crystal phase transformations take place in the thin films or photonic structures, and the accompanying volume reduction as well as the burn-out of residual impurities can lead to mechanical instability. The introduction of cation doping (e.g., Al or Nb) in bulk TiO parts is known to alter phase transitions and to stabilize crystalline phases. In this work, we have developed low-temperature ALD super-cycles to introduce AlO into TiO thin films and photonic crystals. The aluminum oxide content was adjusted by varying the TiO:AlO internal loop ratio within the ALD super-cycle. Both thin films and inverse opal photonic crystal structures were subjected to thermal treatments ranging from 200 to 1200 °C and were characterized by in- and ex-situ X-ray diffraction, spectroscopic ellipsometry, and spectroscopic reflectance measurements. The results show that the introduction of alumina affects the crystallization and phase transition temperatures of titania as well as the optical properties of the inverse opal photonic crystals (iPhC). The thermal stability of the titania iPhCs was increased by the alumina introduction, maintaining their photonic bandgap even after heat treatment at 900 °C and outperforming the pure titania, with the best results being achieved with the super-cycles corresponding to an estimated alumina content of 26 wt.%.

摘要

通过原子层沉积(ALD)在低温(<100°C)下沉积的TiO薄膜通常是非晶态的,与它们的晶体对应物相比,其折射率较小。然而,当基板或模板基于聚合物材料时,需要低温ALD,因为沉积必须在其玻璃化转变温度或熔点以下进行。通过自组装聚苯乙烯模板的ALD渗透生成光子晶体时就是这种情况。当加热时,薄膜或光子结构中会发生晶相转变,伴随的体积减小以及残留杂质的烧尽会导致机械不稳定性。已知在块状TiO部件中引入阳离子掺杂(例如Al或Nb)会改变相变并稳定晶相。在这项工作中,我们开发了低温ALD超循环,将AlO引入TiO薄膜和光子晶体中。通过改变ALD超循环内的TiO:AlO内环比来调整氧化铝含量。薄膜和反蛋白石光子晶体结构都经过了200至1200°C的热处理,并通过原位和非原位X射线衍射、光谱椭偏仪和光谱反射率测量进行了表征。结果表明,氧化铝的引入会影响二氧化钛的结晶和相变温度以及反蛋白石光子晶体(iPhC)的光学性质。氧化铝的引入提高了二氧化钛iPhC的热稳定性,即使在900°C热处理后仍能保持其光子带隙,并且优于纯二氧化钛,对应于估计氧化铝含量为26 wt.%的超循环取得了最佳结果。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2101/8074236/0dea8f8f322d/nanomaterials-11-01053-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2101/8074236/aeddce84c936/nanomaterials-11-01053-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2101/8074236/7acbb5709825/nanomaterials-11-01053-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2101/8074236/4ca6403ddc02/nanomaterials-11-01053-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2101/8074236/bde097756a3f/nanomaterials-11-01053-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2101/8074236/0f22dcaf330b/nanomaterials-11-01053-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2101/8074236/0dea8f8f322d/nanomaterials-11-01053-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2101/8074236/aeddce84c936/nanomaterials-11-01053-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2101/8074236/7acbb5709825/nanomaterials-11-01053-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2101/8074236/4ca6403ddc02/nanomaterials-11-01053-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2101/8074236/bde097756a3f/nanomaterials-11-01053-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2101/8074236/0f22dcaf330b/nanomaterials-11-01053-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2101/8074236/0dea8f8f322d/nanomaterials-11-01053-g006.jpg

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