Here, the first term, V GS S ψ ∂ ∂ , known as the "body factor", cannot be less than 1 for standard MOSFET electrostatics, and the second term log I ( ) S 10 D ψ ∂ ∂ that is equals ln(10) β K T q and is 60 mV dec −1 at room temperature, determines the minimum limit of the subthreshold swing for the thermionic emission over the Boltzmann barrier. This in turn defines the steepness/slope of the transfer curves, the signal gain and the dynamic power dissipation of the electronic switches. One way to circumvent this limit is to allow tunneling through the barrier; in this case band-to-band-tunneling (BTBT) would be required as single career tunneling cannot lead to subthermionic transport. [2] However, the BTBT field-effect transistors (FETs) typically show low Oncurrents; while there are large number of subthermionic tunnel FETs reported in the literature, [3][4][5][6][7][8][9][10][11][12][13] the recent ones based on 2D dichalcogenides demonstrate particularly high performance. [2,14,15] An alternative approach to achieve subthermionic transport, originally proposed by Salahuddin and Datta [16] and later experimentally demonstrated by various research groups, [16][17][18][19][20][21][22][23][24][25][26][27] deals with concept that can actually reduce the body factor to values less than 1. This involves stabilizing a negative capacitance regime by placing a ferroelectric and dielectric layer in series to comprise the MOS capacitor. In this case, the Boltzmann activation barrier remains intact; however, an artificial voltage amplifier or step-up transformer is created using the sharp switching of the dipoles (i.e., exploiting the square-shaped P-E loop) of the ferroelectric and thereby a faster change in Ψ S (surface potential) becomes possible, as compared to the applied ∂V GS . However, in either of these approaches, specific requirements in terms of semiconductors (e.g., single sheet of 2D material), dielectrics or interfaces (e.g., ferroelectric/dielectric interface in case of negative capacitance (NC)-gate FETs) are there, which are certainly nontrivial to be replicated, when the complete device is to be solution processed/printed. Consequently, subthermionic transport Subthreshold slope of field-effect transistors (FETs) less than the fundamental Boltzmann limit (60 mV dec −1 at 300 K) is demonstrated either using band-to-band tunneling or negative capacitance (NC) ferroelectric-gate transistors. However, it is difficult to replicate both of these strategies in solution-processed/printed FETs. Nonetheless, it is shown that the use of a metal-insulator-metal-semiconductor architecture alongside electrolyte gating can simultaneously create highly reproducible static negative capacitance behavior in printed FETs, resulting in subthermionic transport for over four decades of drain currents with a subthreshold slope as low as 16 mV dec −1 , and thereafter a strong thermionic transport regime, characterized by an unprecedented On-current of 195 µA µm −1 , a transconductance of 215 µS µm, and a metal-like On-state res...