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| 001 | 851662 | ||
| 005 | 20210129234955.0 | ||
| 024 | 7 | _ | |a 10.1063/1.5026063 |2 doi |
| 024 | 7 | _ | |a 2128/19664 |2 Handle |
| 024 | 7 | _ | |a WOS:000431141500006 |2 WOS |
| 037 | _ | _ | |a FZJ-2018-05212 |
| 082 | _ | _ | |a 620 |
| 100 | 1 | _ | |a Kindsmüller, A. |0 0000-0001-6236-7391 |b 0 |e Corresponding author |
| 245 | _ | _ | |a Valence change detection in memristive oxide based heterostructure cells by hard X-ray photoelectron emission spectroscopy |
| 260 | _ | _ | |a Melville, NY |c 2018 |b AIP Publ. |
| 336 | 7 | _ | |a article |2 DRIVER |
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| 520 | _ | _ | |a The switching mechanism of valence change resistive memory devices is widely accepted to be an ionic movement of oxygen vacancies resulting in a valence change of the metal cations. However, direct experimental proofs of valence changes in memristive devices are scarce. In this work, we have employed hard X-ray photoelectron emission microscopy (PEEM) to probe local valence changes in Pt/ZrOx/Ta memristive devices. The use of hard X-ray radiation increases the information depth, thus providing chemical information from buried layers. By extracting X-ray photoelectron spectra from different locations in the PEEM images, we show that zirconia in the active device area is reduced compared to a neighbouring region, confirming the valence change in the ZrOx film during electroforming. Furthermore, we succeeded in measuring the Ta 4f spectrum for two different resistance states on the same device. In both states, as well as outside the device region, the Ta electrode is composed of different suboxides without any metallic contribution, hinting to the formation of TaOx during the deposition of the Ta thin film. We observed a reduction of the Ta oxidation state in the low resistance state with respect to the high resistive state. This observation is contradictory to the established model, as the internal redistribution of oxygen between ZrOx and the Ta electrode during switching would lead to an oxidation of the Ta layer in the low resistance state. Instead, we have to conclude that the Ta electrode takes an active part in the switching process in our devices and that oxygen is released and reincorporated in the ZrOx/TaOx bilayer during switching. This is confirmed by the degradation of the high resistance state during endurance measurements under vacuum. |
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| 700 | 1 | _ | |a Schmitz, C. |0 P:(DE-Juel1)159492 |b 1 |
| 700 | 1 | _ | |a Wiemann, C. |0 P:(DE-Juel1)131035 |b 2 |
| 700 | 1 | _ | |a Skaja, K. |0 P:(DE-Juel1)145428 |b 3 |
| 700 | 1 | _ | |a Wouters, D. J. |0 0000-0002-6766-8553 |b 4 |
| 700 | 1 | _ | |a Waser, R. |0 P:(DE-Juel1)131022 |b 5 |
| 700 | 1 | _ | |a Schneider, C. M. |0 P:(DE-Juel1)130948 |b 6 |
| 700 | 1 | _ | |a Dittmann, R. |0 P:(DE-Juel1)130620 |b 7 |e Corresponding author |
| 773 | _ | _ | |a 10.1063/1.5026063 |g Vol. 6, no. 4, p. 046106 - |0 PERI:(DE-600)2722985-3 |n 4 |p 046106 - |t APL materials |v 6 |y 2018 |x 2166-532X |
| 856 | 4 | _ | |u https://juser.fz-juelich.de/record/851662/files/1.5026063.pdf |y OpenAccess |
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