Enhanced negative capacitance in La-doped Pb(Zr0.4Ti0.6)O3 ferroelectric capacitor from tuning of bias voltage pulse

G Ganga S. Kumar (Multiscale Microstructure and Mechanics of Materials Division, CSIR-Central Glass and Ceramic Research Institute 1 , Kolkata 700032,) S Sudipta Goswami (School of Materials Science and Nanotechnology, Jadavpur University 2 , Kolkata 700032,) S Subhashree Chatterjee (DOD Center of Excellence for Advanced Electro-Photonics with 2D Materials, Morgan State University 1 , Baltimore, Maryland 21251,) D Dilruba Hasina (School of Physical Sciences, Indian Association for the Cultivation of Science 1 , 2A & 2B Raja S. C. Mullick Road, Kolkata 700032,) M Miral Verma (School of Minerals, Metallurgical and Materials Engineering, Indian Institute of Technology 4 , Bhubaneswar 752050,) D Devajyoti Mukherjee (School of Physical Sciences, Indian Association for the Cultivation of Science 1 , 2A & 2B Raja S. C. Mullick Road, Kolkata 700032,) C Chandan Kumar Ghosh (School of Materials Science and Nanotechnology, Jadavpur University 2 , Kolkata 700032,) D Dipten Bhattacharya (Multiscale Microstructure and Mechanics of Materials Division, CSIR-Central Glass and Ceramic Research Institute 1 , Kolkata 700032,)

Abstract

We report a remarkable bias voltage dependent specific negative capacitance in multidomain La-doped Pb[Zr0.4Ti0.6)O3(PLZT)] ferroelectric capacitors. The specific negative capacitance maximizes at a specific bias voltage because of emergence of maximum domain-wall density during “switching” of the domains. Domain configuration changes from such an “optimum” state if higher or lower bias voltage is applied at a much faster or slower rate. Phase-field simulation using time-dependent Ginzburg–Landau equation corroborates the experimental results and shows dependence of the domain-wall length during switching on the bias voltage amplitude and its maximization at a specific bias voltage amplitude. Interestingly, the radius of curvature of the resulting polarization (P) vs voltage (V) hysteresis loop at the coercive voltage (VC), as well, turns out to be depending on the bias voltage. All these results indicate a close correlation among the bias voltage pulse profile (amplitude and time scale), domain-wall length during switching, shape of the resulting ferroelectric hysteresis loop, and the transient negative capacitance. It may have important ramifications both in the context of physics behind negative capacitance in a multidomain ferroelectric capacitor and devices being developed by exploiting its advantages.

Article Details

Volume / Issue Vol. 139, Issue 3
Published January 21, 2026
ISSN 0021-8979
Publisher American Institute of Physics

Journal Info

Journal of Applied Physics

American Institute of Physics

ISSN: 0021-8979 Physical Sciences

Authors (8)

G

Ganga S. Kumar

Multiscale Microstructure and Mechanics of Materials Division, CSIR-Central Glass and Ceramic Research Institute 1 , Kolkata 700032,

S

Sudipta Goswami

School of Materials Science and Nanotechnology, Jadavpur University 2 , Kolkata 700032,

S

Subhashree Chatterjee

DOD Center of Excellence for Advanced Electro-Photonics with 2D Materials, Morgan State University 1 , Baltimore, Maryland 21251,

D

Dilruba Hasina

School of Physical Sciences, Indian Association for the Cultivation of Science 1 , 2A & 2B Raja S. C. Mullick Road, Kolkata 700032,

M

Miral Verma

School of Minerals, Metallurgical and Materials Engineering, Indian Institute of Technology 4 , Bhubaneswar 752050,

D

Devajyoti Mukherjee

School of Physical Sciences, Indian Association for the Cultivation of Science 1 , 2A & 2B Raja S. C. Mullick Road, Kolkata 700032,

C

Chandan Kumar Ghosh

School of Materials Science and Nanotechnology, Jadavpur University 2 , Kolkata 700032,

D

Dipten Bhattacharya

Multiscale Microstructure and Mechanics of Materials Division, CSIR-Central Glass and Ceramic Research Institute 1 , Kolkata 700032,