Related Experiment Video
Updated: May 14, 2026

A Fabrication and Measurement Method for a Flexible Ferroelectric Element Based on Van Der Waals Heteroepitaxy
Published on: April 8, 2018
Unified Steep-Slope Switching and Non-Volatile Memory in a Complementarily Stabilized van der Waals Ferroelectric
Sangmin Lee1, Stanislav Sin2, Cheolhwa Jang1
1SKKU Advanced Institute of Nanotechnology (SAINT), Sungkyunkwan University, Suwon, South Korea.
None:
Achieving both steep-slope switching and robust non-volatile memory within a single transistor would enable new device concepts for low-power and logic-in-memory architectures. Conventional negative-capacitance FETs (NC-FETs) are designed to suppress ferroelectric bistability to enable hysteresis-free sub-thermionic switching, whereas ferroelectric FETs (Fe-FETs) exploit bistable polarization to provide non-volatile memory, leaving the two operating regimes largely separate in practice. Here, we report a van der Waals ferroelectric negative-capacitance transistor (FeNC-FET) that simultaneously realizes stabilized negative capacitance and intrinsic bistable polarization by employing a CIPS/h-BN/α-In2Se3 trilayer gate stack. Landau-Khalatnikov analysis and polarization-voltage measurements confirm complementary ferroelectric roles in which CIPS provides static negative curvature, h-BN enables charge compensation, and α-In2Se3 supplies non-volatile polarization. This cooperative mechanism enables steep sub-threshold swings of 35 mV/dec (forward) and 51 mV/dec (reverse), a ∼3 V memory window, long retention (>104 s), and endurance exceeding 2500 cycles. The device further performs AND, OR, and majority logic-in-memory operations using 10 µs pulses with clear ON/OFF separation. These results establish the FeNC-FET as a compact platform that combines steep-slope switching with non-volatile programmability in a single device, enabling low-bias readout, short-pulse programming, and robust logic-in-memory operation.
Related Concept Videos
MOS Capacitor
The metal gate is typically made from highly conductive materials such as aluminum or polysilicon. Beneath the metal gate lies a thin layer of...
Biasing of FET
In an N-channel JFET, the structure consists of N-type material forming the channel on a P-type substrate, with the gate...
MOSFET: Enhancement Mode
In their basic form, enhancement-mode MOSFETs are typically non-conductive when the gate-source voltage (Vgs) is zero. This default 'off' state means no current...
Biasing of Metal-Semiconductor Junctions
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
Metal-Semiconductor Junctions
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The semiconductor's...
Types of Semiconductors

