Instability Mechanism for STT-MRAM switching

TL;DR

This paper investigates the primary switching mechanism in STT-MRAM, demonstrating that a global magnetostatic instability, rather than local nucleation, dominates the switching process in larger, thermally stable elements.

Contribution

The study visualizes switching trajectories to identify the dominant mechanism, providing evidence that magnetostatic instability, not local nucleation, governs switching in STT-MRAM.

Findings

Switching follows quasi-uniform precession until a critical amplitude.

Magnetostatic instability leads to domain wall formation and completes switching.

Local edge nucleation was unsuccessfully induced, indicating it is not the primary mechanism.

Abstract

To optimize the design of STT-MRAM (spin-transfer torque magnetic random access memory), it is necessary to be able to predict switching (error) rates. For small elements, this can be done using a single-macrospin theory since the element will switch quasi-uniformly. Experimental results on switching rates suggest that elements large enough to be thermally stable switch by some mechanism with a lower energy barrier. It has been suggested that this mechanism is local nucleation, but we have also previously reported a global magnetostatic instability, which is consistent with the lower experimental energy barriers. In this paper, we try to determine which of these mechanisms is most important by visualizing the switching in a "U-NU" (uniform - nonuniform) phase diagram. We find that switching trajectories follow the horizontal U axis (i.e., quasi-uniform precession) until they reach a critical amplitude, at which the magnetostatic instability grows exponentially and a domain wall forms at the center, whose motion completes the switching. We have tried unsuccessfully to induce local nucleation (a domain wall at the edge). We conclude that the dominant switching mechanism is not edge nucleation, but the magnetostatic instability.