Abstract

Tunneling field-effect transistors (TFETs) are of considerable interest owing to their capability of low-power operation. Here, we demonstrate a novel type of TFET which is composed of a thin black phosphorus–tin diselenide (BP–SnSe2) heterostructure. This combination of 2D semiconductor thin sheets enables device operation either as an Esaki diode featuring negative differential resistance (NDR) in the negative gate voltage regime or as a backward diode in the positive gate bias regime. Such tuning possibility is imparted by the fact that only the carrier concentration in the BP component can be effectively modulated by electrostatic gating, while the relatively high carrier concentration in the SnSe2 sheet renders it insensitive against gating. Scanning photocurrent microscopy maps indicate the presence of a staggered (type II) band alignment at the heterojunction. The temperature-dependent NDR behavior of the devices is explainable by an additional series resistance contribution from the individual BP and SnSe2 sheets connected in series. Moreover, the backward rectification behavior can be consistently described by the thermionic emission theory, pointing toward the gating-induced formation of a potential barrier at the heterojunction. It furthermore turned out that for effective Esaki diode operation, care has to be taken to avoid the formation of positive charges trapped in the alumina passivation layer.

Highlights

  • Modern electronic applications require integrated circuits of substantially reduced dynamic and static power consumption

  • We have successfully fabricated thin black phosphorus (BP)−SnSe2 p− n heterostructure devices whose operation mode is tunable by electrostatic gating between the negative differential resistance (NDR) and backward diode regime

  • This tuning is enabled by the fact that application of a global back-gate predominantly affects the thin BP sheet because if its lower charge carrier density in comparison to the SnSe2 sheets

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Summary

■ INTRODUCTION

Modern electronic applications require integrated circuits of substantially reduced dynamic and static power consumption. In close correspondence to a previous report on a bulk BP−SnSe2 heterojunction,[29] we observed NDR behavior and positive photocurrent for a bulk BP−SnSe2 heterojunction device, implying type III (broken-gap) band alignment in this case (see the Supporting Information for further details) First of all, this difference between the bulk and few-layer heterostructure likely originates from a thickness-dependent carrier density of BP, that is, a decreased doping concentration with decreasing BP thickness.[32] In the device comprising bulk BP, while the high carrier concentration principally favors the TFET operation, the resulting poor gate controllability is a significant drawback. This finding is in accord with the absence of fixed surface charges on PMMA, underlining the importance of properly choosing the passivation layer and its fabrication conditions

■ CONCLUSIONS
■ METHODS
■ ACKNOWLEDGMENTS
■ REFERENCES
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