Boltzmann distribution thermal tails of carriers restrain
the subthreshold
swing (SS) of field-effect transistors (FETs) to be lower than 60
mV/decade at room temperature, which restrains the reduction of operate-voltage
and power consumption of transistors. The negative-capacitance FET
(NC FET) is expected to break through this physical limit and obtain
a steep SS by amplifying the gate voltage through the negative capacitance
effect of the ferroelectric thin film, providing a new way to further
reduce the power consumption of the transistor at the end of Moore’s
law. Here, we show a MoS2 NC FET with a CuInP2S6 ferroelectric, exhibiting a large on/off ratio of 108, a steep SS as low as 6 mV/decade, and a wide sub-60 mV/decade
drain current range of more than 4 orders of magnitude while sacrificially
inducing a huge hysteresis larger than 500 mV. Furthermore, we found
that by inserting the h-phase boron nitride (h-BN) layer with suitable
thickness, the dielectric capacitance matches the ferroelectric negative
capacitance better, and thus the hysteresis on the transfer curve
is reduced, and the ideal switching-behavior transistors with SS as
low as 62 mV/decade and only 5 mV negligible hysteresis were obtained.
Our work demonstrates that under the capacitance–matching condition,
the hysteresis-free negative-capacitance transistors do not act as
the predicted steep-slope transistors, but their voltage-saving still
occurs instead as a type of effective transconductance booster with
more than 20 times transconductance amplification.