Correlation between Electronic Structure, Microstructure, and Switching Mode in Valence Change Mechanism Al2O3/TiOx‐Based Memristive Devices

Author:

Aussen Stephan12ORCID,Cüppers Felix1ORCID,Funck Carsten1,Jo Janghyun3ORCID,Werner Stephan4ORCID,Pratsch Christoph4ORCID,Menzel Stephan1ORCID,Dittmann Regina1ORCID,Dunin‐Borkowski Rafal3ORCID,Waser Rainer15ORCID,Hoffmann‐Eifert Susanne1ORCID

Affiliation:

1. Peter Grünberg Institut (PGI 7 and 10) and JARA‐FIT Forschungszentrum Jülich GmbH Wilhelm‐Johnen‐Straße 52428 Jülich Germany

2. RWTH Aachen University Templergraben 55 52062 Aachen Germany

3. Ernst Ruska‐Center (ERC‐1 / PGI‐5) and JARA‐FIT Forschungszentrum Jülich GmbH Wilhelm‐Johnen‐Straße 52428 Jülich Germany

4. Department X‐ray Microscopy Helmholtz‐Zentrum für Materialien und Energie GmbH Albert‐Einstein‐Str. 15 12489 Berlin Germany

5. Institute of Materials in Electrical Engineering and Information Technology II RWTH Aachen University Sommerfeldstraße 24 52074 Aachen Germany

Abstract

AbstractMemristive devices with valence change mechanism (VCM) show promise for neuromorphic data processing, although emulation of synaptic behavior with analog weight updates remains a challenge. Standard filamentary and area‐dependent resistive switching exhibit characteristic differences in the transition from the high to low resistance state, which is either abrupt with inherently high variability or gradual and allows quasi‐analog operation. In this study, the two switching modes are clearly correlated to differences in the microstructure and electronic structure for Pt/Al2O3/TiOx/Cr/Pt devices made from amorphous layers of 1.2 nm Al2O3 and 7 nm TiOx by atomic layer deposition. For the filamentary mode, operando spectromicroscopy experiments identify a localized region of ≈50 nm in diameter of reduced titania surrounded by crystalline rutile‐like TiO2, highlighting the importance of Joule heating for this mode. In contrast, both oxide layers remain in their amorphous state for the interfacial mode, which proves that device temperature during switching stays below 670 K, which is the TiO2 crystallization temperature. The analysis of the electronic conduction behavior confirms that the interfacial switching occurs by modulating the effective tunnel barrier width due to accumulation and depletion of oxygen vacancies at the Al2O3/TiOx interface. The results are transferable to other bilayer stacks.

Funder

Bundesministerium für Bildung und Forschung

Deutsche Forschungsgemeinschaft

Publisher

Wiley

Subject

Electronic, Optical and Magnetic Materials

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