Polarity dependent predictable and random resistive switching in forming-free unipolar memristors

GND
1280829451
ORCID
0009-0000-7362-2896
Zugehörigkeit
Leibniz Institute of Photonic Technology, Jena
Rayapati, Venkata Rao;
GND
1217627359
ORCID
0000-0002-1977-1206
Zugehörigkeit
Leibniz Institute of Photonic Technology, Jena
Vegesna, Sahitya Varma;
GND
1217627146
ORCID
0009-0002-9185-3967
Zugehörigkeit
Leibniz Institute of Photonic Technology, Jena
Bhat, Vinayak Jayram;
GND
1192700961
ORCID
0000-0002-7407-0453
Zugehörigkeit
Leibniz Institute of Photonic Technology, Jena
Blaschke, Daniel;
GND
1316657558
ORCID
0009-0006-8748-3392
Zugehörigkeit
Leibniz Institute of Photonic Technology, Jena
Diegel, Marco;
GND
135981941X
ORCID
0009-0009-5611-4588
Zugehörigkeit
Leibniz Institute of Photonic Technology, Jena
Dellith, Andrea;
GND
135947227
ORCID
0009-0008-0930-4437
Zugehörigkeit
Leibniz Institute of Photonic Technology, Jena
Dellith, Jan;
ORCID
0000-0003-0685-5301
Zugehörigkeit
Institute of Ion Beam Physics and Materials Research, Helmholtz-Zentrum Dresden-Rossendorf e.V., 01328 Dresden
Bürger, Danilo;
Zugehörigkeit
Institute of Ion Beam Physics and Materials Research, Helmholtz-Zentrum Dresden-Rossendorf e.V., 01328 Dresden
Skorupa, Ilona;
GND
121791939
ORCID
0000-0001-7100-6926
Zugehörigkeit
Leibniz Institute of Photonic Technology, Jena
Schmidt, Heidemarie

Polycrystalline, hexagonal HoMnO3 thin films sandwiched between an un-patterned Pt/Ti bottom electrode and a circularly patterned Al top electrode reveal forming-free, polarity dependent predictable and random, unipolar resistive switching with stable retention, and a resistance ratio between high resistance state (HRS) and low resistance state (LRS) larger than 104. An equivalent circuit model is proposed to describe the HoMnO3 memristor as a three-layered capacitor structure. Based on the energy band diagram of the HoMnO3 structure under applied negative and positive write bias, polarity dependent, predictable, and random resistive switching is explained. Furthermore, the conductance in LRS until RESET and in HRS until SET has been investigated. The conductance in LRS is large and constant until RESET bias is reached. The conductance in HRS increases from nearly zero to quantum conductance G0 (2e2/h) until SET bias is reached.

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