期刊
APPLIED PHYSICS LETTERS
卷 118, 期 1, 页码 -出版社
AIP Publishing
DOI: 10.1063/5.0029532
关键词
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资金
- National Science Foundation, Center for Dielectrics and Piezoelectrics [IIP-1841453, IIP-1841466]
- National Science Foundation [DGE-1746939, DGE-1842490, ECCS-2025064]
- Semiconductor Research Corporation's Global Research Collaboration program [2875.001]
- State of North Carolina
The study introduces a new ALD technique SNAP to fabricate ferroelectric Hf0.5Zr0.5O2 capacitors and reveals different ferroelectric behaviors depending on the annealing temperature. Analysis of XRD patterns and depth profiling suggests differences between TiN and Hf0.5Zr0.5O2 layers made via SNAP deposition, potentially impacting the performance of the capacitors.
We introduce an Atomic Layer Deposition (ALD) technique referred to here as Sequential, No-Atmosphere Processing (SNAP) to fabricate ferroelectric Hf0.5Zr0.5O2 capacitors in Metal-Ferroelectric-Metal (MFM) structures. SNAP involves the ALD of each layer sequentially while maintaining the sample under vacuum process conditions without ambient exposure during the entire sequential deposition processes. We first use plasma enhanced ALD to fabricate 002-textured TiN films and study the degree of texture and quality of the film by X-ray Diffraction (XRD), Time-of-Flight Secondary Ion Mass Spectrometry (ToF-SIMS), and transmission electron microscopy. Building upon the textured TiN film, we fabricate MFM capacitors with 10-nm-thick Hf0.5Zr0.5O2 via SNAP deposition and observe an unexpectedly large remanent polarization (2P(r)=54.2 mu C/cm(2)). We report that annealing at T<800C and at T=800 degrees C results in different ferroelectric behaviors and phases determined by grazing incidence XRD patterns. We infer that the nonpolar tetragonal phase is dominant in films treated at T<800C, whereas the polar orthorhombic phase is dominant in films treated at T=800 degrees C. Using ToF-SIMS and x-ray spectroscopy depth profiling on MFM capacitors, we observe an increase in the concentration of defects in the Hf0.5Zr0.5O2 layer after annealing. We believe that the absence of the native passive layer between Hf0.5Zr0.5O2 and TiN layers made via SNAP deposition is responsible for the unexpectedly large remanent polarization. In addition, we associate the 002-textured TiN as potentially playing a role in realizing the unexpectedly large remanent polarization.
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