Introduction
Magnetic tunnel junctions (MTJs) have emerged as the building blocks of spintronic circuits due to their large tunneling magnetoresistance (TMR) ratios, and the possibility of integration with conventional semiconductor electronics. The use of spin-polarized currents to switch magnetization in MTJs, e.g., via spin-transfer-torque (STT), however, limits the energy efficiency and density of STT-based MRAM, due to Ohmic losses and the need for large transistors to drive the required switching current, respectively (1). Therefore, electric-field control of magnetism could result not only in a magnetoelectric random access memory (MeRAM) with improved energy efficiency and density compared to STT-RAM, but also in new applications for nonvolatile spintronic devices, by making them energetically competitive compared to traditional semiconductor solutions for logic and computation.