December 1 - 6, 2024
Boston, Massachusetts

Event Supporters

2024 MRS Fall Meeting & Exhibit
EL03.09.01

2D Materials for Neuromorphic Computing Devices

When and Where

Dec 4, 2024
9:15am - 9:45am
Sheraton, Second Floor, Back Bay C

Presenter(s)

Co-Author(s)

Max Lemme1,2

RWTH Aachen University1,AMO GmbH2

Abstract

Max Lemme1,2

RWTH Aachen University1,AMO GmbH2
2D Materials are one of several material classes considered for resistive switching (RS) devices, potential game-changers for neuromorphic computing hardware <sup>[1]</sup>. Such ”memristive” devices can be switched between two or more resistive states in a volatile or non-volatile way <sup>[2]</sup>, and may be used in computing-in-memory architectures <sup>[3]</sup>, cross-bar arrays <sup>[4]</sup>, or as electronic synapses <sup>[5]</sup>.<br/><br/>Semiconducting molybdenum disulfide (MoS<sub>2</sub>) has been investigated intensively as a RS material. The physical origin of the switching has been attributed to different mechanisms: bias-induced migration of sulfur vacancies and grain boundaries, lattice distortion, reversible modulation of MoS<sub>2</sub> phases, and ion migration. Here, I will discuss different MoS<sub>2</sub> device configurations that depend on the material growth conditions and lead to different RS behavior and mechanisms.<br/><br/>Cross-point devices, where two metal electrodes are separated by one or several MoS<sub>2</sub> layers oriented perpendicular to the electrodes, are probably the best-studied devices. We show that the choice of electrodes and even the choice of their deposition method can influence the switching behavior and reliability. In particular, metal-organic chemical vapor deposited (MOCVD) MoS<sub>2</sub> with sputtered Al top-electrodes show significantly reduced variability, with high yields of up to 95% and competitive endurance, retention, and switching speeds compared to the state-of-the-art <sup>[6]</sup>.<br/><br/>Vertical MoS<sub>2</sub> films can be grown under certain conditions by thermal conversion of thin molybdenum films. Here, the van der Waals gaps between the vertical layers facilitate electric-field-driven ion movement <sup>[7]</sup>, leading to non-volatile RS. I will show volatile RS in a device combining a SiOx layer with vertically aligned MoS<sub>2</sub>. The devices exhibit repeatable threshold switching at low switching voltages below 1 V, switching times below 400 ns, and endurance of close to 6000 cycles <sup>[8]</sup>.<br/>Similar ion transport in van der Waals gaps can be observed in lateral two-terminal devices based on MOCVD MoS<sub>2</sub>. I will show experiments on silver (Ag) ion migration in lateral MoS<sub>2</sub> memristors that do not require higher “forming” voltages for their initial RS event. These Pd/MoS<sub>2</sub>/Ag devices show volatile switching with ultra-low threshold voltages of 0.3 V and 100-600 ns switching <sup>[9]</sup>.<br/><br/>Furthermore, I will present a study on the current conduction mechanism in memristors with MOCVD-grown hexagonal boron nitride (h-BN) as the active material. The devices were electrically measured in their low and high resistance states in a wide range of temperatures. We propose the formation and retraction of nickel filaments along boron defects as the RS mechanism, with defect-mediated transport in the high resistive state. The devices exhibit low cycle-to-cycle variability of 5% and a large On/Off current ratio of 10<sup>7 [10]</sup>.<br/><br/>Finally, I will discuss the parasitic effect of resist residues, which could potentially lead to misinterpretations of RS in 2D materials <sup>[11]</sup>.<br/><br/>All experiments are corroborated with transmission electron microscopy, Raman spectroscopy, and through other analytical means. <br/><br/>This work has received funding from the German BMBF through grants 03ZU1106xx (NeuroSys) and 16ME0399/16ME0400 (NEUROTEC II).<br/> <br/>[1] M.C. Lemme et al., <i>Nat </i><i>Comm</i> <b>2022</b>, <i>13</i>, 1392.<br/>[2] D.B. Strukov et al., <i>Nat Electron</i> <b>2018</b>, <i>1</i>, 333.<br/>[4] S. Chen et al., <i>Nat Electron</i> <b>2020</b>, <i>3</i>, 638.<br/>[5] G. Zhou et al., <i>Adv Electron Mat</i> <b>2022</b>, <i>8</i>, 2101127.<br/>[6] D. Braun et al., in <i>Device Research Conference (DRC)</i>, College Park, Maryland, USA, <b>2024</b>.<br/>[7] M. Belete et al., <i>Adv Electro Mat</i> <b>2020</b>, 1900892.<br/>[8] J. Lee et al., <i>Device Research Conference (DRC)</i>, College Park, Maryland, USA, <b>2024</b>.<br/>[9] S. Cruzes et al., <i>Device Research Conference (DRC)</i>, College Park, Maryland, USA, <b>2024</b>.<br/>[10] L. Völkel et al., <i>Adv Funct Mat</i> <b>2024</b>, <i>34</i>, 2300428.<br/>[11] D. Braun et al., <b>2023</b>, DOI 10.48550/arXiv.2309.13900.

Symposium Organizers

Deji Akinwande, The University of Texas at Austin
Cinzia Casiraghi, University of Manchester
Carlo Grazianetti, CNR-IMM
Li Tao, Southeast University

Session Chairs

Cinzia Casiraghi
Cecilia Mattevi

In this Session