Pulse length and amplitude dependent resistive switching mechanisms in Pt-Pr0.67Ca0.33MnO3-Pt sandwich structures

We report here on the presence of two different nonvolatile resistive switching mechanisms in Pt-Pr _0.67 Ca _0.33 MnO _3 -Pt sandwich structures based on pulsed electrical transport measurements. As a function of pulse length, amplitude and temperature, the devices show two different switching regi...

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Main Authors: M Scherff, B Meyer, J Hoffmann, C Jooss, M Feuchter, M Kamlah
Format: Article
Language:English
Published: IOP Publishing 2015-01-01
Series:New Journal of Physics
Subjects:
Online Access:https://doi.org/10.1088/1367-2630/17/3/033011
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author M Scherff
B Meyer
J Hoffmann
C Jooss
M Feuchter
M Kamlah
author_facet M Scherff
B Meyer
J Hoffmann
C Jooss
M Feuchter
M Kamlah
author_sort M Scherff
collection DOAJ
description We report here on the presence of two different nonvolatile resistive switching mechanisms in Pt-Pr _0.67 Ca _0.33 MnO _3 -Pt sandwich structures based on pulsed electrical transport measurements. As a function of pulse length, amplitude and temperature, the devices show two different switching regimes. The first is positive switching (PS) where a high resistance state (HRS) evolves at positive bias at the top electrode in the voltage range of U  ≈ 0.5–1.2 V and pulse lengths t _p  ≈ 10 ^−7 s. In addition, we observe a cross over to negative switching (NS) for U  > 1 V and t _p  ≈ 10 ^−3 s. Here, the HRS evolves at negative bias applied at the top electrode. We present strong evidence that both switching mechanisms take place at the interface between Pr _0.67 Ca _0.33 MnO _3 and the top electrode. Based on finite element simulations of the temperature evolution during the electrical pulses, we show that the onset of Joule heating is characteristic of the PS regime, whereas drastic temperature increases of several hundred Kelvin evolve during NS. Based on the observed different timescales, pulse amplitudes and temperature dependences of PS and NS, respectively, we suggest that two different switching mechanisms are involved: a fast, short range exchange of oxygen at the interface with the metallic electrode for PS and a slower, long range redistribution of oxygen in the entire PCMO film for the NS.
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spelling doaj.art-f115b0f7efd84770a97a11aa7aab2e012023-08-08T14:19:13ZengIOP PublishingNew Journal of Physics1367-26302015-01-0117303301110.1088/1367-2630/17/3/033011Pulse length and amplitude dependent resistive switching mechanisms in Pt-Pr0.67Ca0.33MnO3-Pt sandwich structuresM Scherff0B Meyer1J Hoffmann2C Jooss3M Feuchter4M Kamlah5Institute of Materials Physics, University of Goettingen , D-37077 Goettingen, GermanyInstitute of Materials Physics, University of Goettingen , D-37077 Goettingen, GermanyInstitute of Materials Physics, University of Goettingen , D-37077 Goettingen, GermanyInstitute of Materials Physics, University of Goettingen , D-37077 Goettingen, GermanyKarlsruhe Institute of Technology (KIT), Institute for Applied Materials (IAM), Hermann-von-Helmholtz Platz 1, 76344 Eggenstein-Leopoldshafen, GermanyKarlsruhe Institute of Technology (KIT), Institute for Applied Materials (IAM), Hermann-von-Helmholtz Platz 1, 76344 Eggenstein-Leopoldshafen, GermanyWe report here on the presence of two different nonvolatile resistive switching mechanisms in Pt-Pr _0.67 Ca _0.33 MnO _3 -Pt sandwich structures based on pulsed electrical transport measurements. As a function of pulse length, amplitude and temperature, the devices show two different switching regimes. The first is positive switching (PS) where a high resistance state (HRS) evolves at positive bias at the top electrode in the voltage range of U  ≈ 0.5–1.2 V and pulse lengths t _p  ≈ 10 ^−7 s. In addition, we observe a cross over to negative switching (NS) for U  > 1 V and t _p  ≈ 10 ^−3 s. Here, the HRS evolves at negative bias applied at the top electrode. We present strong evidence that both switching mechanisms take place at the interface between Pr _0.67 Ca _0.33 MnO _3 and the top electrode. Based on finite element simulations of the temperature evolution during the electrical pulses, we show that the onset of Joule heating is characteristic of the PS regime, whereas drastic temperature increases of several hundred Kelvin evolve during NS. Based on the observed different timescales, pulse amplitudes and temperature dependences of PS and NS, respectively, we suggest that two different switching mechanisms are involved: a fast, short range exchange of oxygen at the interface with the metallic electrode for PS and a slower, long range redistribution of oxygen in the entire PCMO film for the NS.https://doi.org/10.1088/1367-2630/17/3/033011resistive switchingPCMOoxygen diffusionJoule heatingfinite element simulationelectrode oxidation
spellingShingle M Scherff
B Meyer
J Hoffmann
C Jooss
M Feuchter
M Kamlah
Pulse length and amplitude dependent resistive switching mechanisms in Pt-Pr0.67Ca0.33MnO3-Pt sandwich structures
New Journal of Physics
resistive switching
PCMO
oxygen diffusion
Joule heating
finite element simulation
electrode oxidation
title Pulse length and amplitude dependent resistive switching mechanisms in Pt-Pr0.67Ca0.33MnO3-Pt sandwich structures
title_full Pulse length and amplitude dependent resistive switching mechanisms in Pt-Pr0.67Ca0.33MnO3-Pt sandwich structures
title_fullStr Pulse length and amplitude dependent resistive switching mechanisms in Pt-Pr0.67Ca0.33MnO3-Pt sandwich structures
title_full_unstemmed Pulse length and amplitude dependent resistive switching mechanisms in Pt-Pr0.67Ca0.33MnO3-Pt sandwich structures
title_short Pulse length and amplitude dependent resistive switching mechanisms in Pt-Pr0.67Ca0.33MnO3-Pt sandwich structures
title_sort pulse length and amplitude dependent resistive switching mechanisms in pt pr0 67ca0 33mno3 pt sandwich structures
topic resistive switching
PCMO
oxygen diffusion
Joule heating
finite element simulation
electrode oxidation
url https://doi.org/10.1088/1367-2630/17/3/033011
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