I. Introduction
Due to the continued scaling of logic devices over the past several decades, several physical limitations have emerged that require the development of novel device structures. In particular, the MOSFET architecture is limited to a subthreshold swing (SS) of 60 mV/decade by the slope of the Fermi function at room temperature. In order to continue scaling the bias voltage and the power consumption of these devices, a smaller SS is necessary, requiring alternative device architectures. Additionally, device scaling has been accompanied by increased OFF state currents and increased power density [1]. Each of these considerations complicates scaling of devices for future technology nodes.