4.8 Article

Origin of Ferroelectricity in Epitaxial Si-Doped HfO2 Films

Journal

ACS APPLIED MATERIALS & INTERFACES
Volume 11, Issue 4, Pages 4139-4144

Publisher

AMER CHEMICAL SOC
DOI: 10.1021/acsami.8b19558

Keywords

PLD; epitaxial Si-doped HfO2 thin films; N-type SrTiO3 substrates; ferroelectricity; XRD; PFM; HRTEM; XAS

Funding

  1. Science and Technology Research Items of Shenzhen [JCYJ20160422102802301, KQJSCX2016022619562452]
  2. National Natural Science Foundation of China [11604214]
  3. Fund of the State Key Laboratory of Solidification Processing in NWPU [SKLSP201615]
  4. Scientific Research Foundation of Advanced Talents (Innovation Team), DGUT [KCYCXPT2016004, KCYKYQD2017013, KCYXIVI2017014, gb-200902-44]
  5. Science and Technology Planning Project of Guangdong [2014A010105058]

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HfO2-based unconventional ferroelectric materials were recently discovered and have attracted a great deal of attention in both academia and industry. The growth of epitaxial Si-doped HfO2 films has opened up a route to understand the mechanism of ferroelectricity. Here, we used pulsed laser deposition to grow epitaxial Si-doped HfO2 films in different orientations of N-type SrTiO3 substrates. Polar nanodomains can be written and read using piezoforce microscopy, and these domains are reversibly switched with a phase change of 180 degrees. Films with different thicknesses displayed a coercive field E-c and a remnant polarization P-r of approximately 4-5 MV/cm and 8-32 mu C/cm(2), respectively. X-ray diffraction and high-resolution transmission electron microscopy (HRTEM) results identified that the as-grown Si-doped HfO2 films have strained fluorite structures. The ABAB stacking mode of the Hf atomic grid observed by HRTEM clearly demonstrates that the ferroelectricity originates from the noncentrosymmetric Pca2(1) polar structure. Combined with soft X-ray absorption spectra, the results showed that the Pca2(1) ferroelectric crystal structure manifested as an O sublattice distortion by the effect of the interface strain and Si dopant interactions, resulting in a nanoscaled ferroelectric ordered state because of further crystal splitting.

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