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. 2022 Mar 9;13:1228. doi: 10.1038/s41467-022-28860-1

Fig. 3. Demonstration of antiferroelectric negative capacitance.

Fig. 3

a Experimental setup of the pulsed charge-voltage measurements on the dielectric-antiferroelectric heterostructure. Vin, VDE-AFE, R and I are the applied voltage pulse, the voltage across the DE-AFE capacitor, the series resistor (5.6 kΩ) and the current through R, respectively. The waveforms of Vin and VDE-AFE were measured using an oscilloscope at different amplitudes of the Vin pulse. b Transient waveforms of Vin, VDE-AFE, I and integrated charge for a HfO2(8 nm)/Al2O3(~ 1 nm)/ZrO2(10 nm) capacitor. c Maximum charge Qmax, residual charge Qres, and reversibly stored charge ΔQ as functions of maximum voltage across the DE-AFE capacitor Va measured from the waveforms shown in b. d Polarization P as a function of extracted electric field Ea across the ZrO2 layer in a HfO2(8 nm)/Al2O3(~ 1 nm)/ZrO2 (10 nm) heterostructure capacitor. The PEa characteristics of an equivalent stand-alone ZrO2 capacitor measured on a conventional ferroelectric tester is also shown for comparison in the background. The negative capacitance regions (CAFE < 0) in the PEa curve correspond to the capacitance enhancement regions in the ΔQ-Va curve shown in c. e Extracted energy landscape of ZrO2. Second derivative of the free energy G with respect to P based on a polynomial fit is shown below.