I. Introduction
The lookout for alternatives to metal oxide field effect transistors (MOSFETs) for low power applications has been met with a number of novel devices in the past two decades [1]-[3]. Of such emerging devices which possess the promises to counter effects of downscaling, tunnel field effect transistors (TFETs) have acquired great attention due to their ability to offer sub-kT/q subthreshold swing (SS) and low leakage current [4]-[6]. The phenomenon of quantum tunneling in TFETs as opposed to thermionic emission in MOSFETs attributes negligible short channel effects to the former. Most commonly a gated reverse-biased p-i-n structure, TFETs come with drawbacks of low on-state current (ION), and acute ambipolarity. There have been many architectures, and techniques proposed so far to tackle these drawbacks. Of them, the double gate TFETs [7], gate-drain underlap TFETs [8], p-n-p-n TFETs [9], halo-pocket TFETs [10], heterojunction TFETs [11], and hetero-gate TFETs [12] are some of the prominent ones.