A Chiral B−N Adduct as a New Frontier in Ferroelectrics and Piezoelectric Energy Harvesting

Author:

Sahoo Supriya1ORCID,Mukherjee Supratik2ORCID,Sharma Vijay Bhan3,Hernández Wilfredo Ibarra4ORCID,Garcia‐Castro Andrés Camilo5ORCID,Zaręba Jan K.6ORCID,Kabra Dinesh3ORCID,Vaitheeswaran Ganapathy7,Boomishankar Ramamoorthy1ORCID

Affiliation:

1. Department of Chemistry and Centre for Energy Science Indian Institute of Science Education and Research, Pune Dr. Homi Bhabha Road Pune 411008 India

2. Advanced Centre of Research in High Energy Materials (ACRHEM) University of Hyderabad Prof. C.R. Rao Road, Gachibowli Hyderabad 500046 Telangana India

3. Department of Physics and Center for Research in Nanotechnology and Sciences Indian Institute of Technology Mumbai 400076 India

4. Facultad de Ingeniería Benemérita Universidad Autónoma de Puebla Apartado Postal J-39 72570 Puebla Puebla México

5. School of Physics Universidad Industrial de Santander Carrera 27 Calle 09 Bucaramanga 680002 Colombia

6. Institute of Advanced Materials Wrocław University of Science and Technology 50-370 Wrocław Poland

7. School of Physics University of Hyderabad, Hyderabad Prof. C.R. Rao Road, Gachibowli Hyderabad Telangana 500046 India

Abstract

AbstractWithin the burgeoning field of electronic materials, B−N Lewis acid‐base pairs, distinguished by their partial charge distribution across boron and nitrogen centers, represent an underexplored class with significant potential. These materials exhibit inherent dipoles and are excellent candidates for ferroelectricity. However, the challenge lies in achieving the optimal combination of hard‐soft acid‐base pairs to yield B−N adducts with stable dipoles. Herein, we present an enantiomeric pair of B−N adducts [R/SC6H5CH(CH3)NH2BF3] (R/SMBA‐BF3) crystallizing in the polar monoclinic P21 space group. The ferroelectric measurements on RMBA‐BF3 gave a rectangular P‐E hysteresis loop with a remnant polarization of 7.65 μC cm−2, a value that aligns with the polarization derived from the extensive density‐functional theory computations. The PFM studies on the drop‐casted film of RMBA‐BF3 further corroborate the existence of ferroelectric domains, displaying characteristic amplitude‐bias butterfly and phase‐bias hysteresis loops. The piezoelectric nature of the RMBA‐BF3 was confirmed by its direct piezoelectric coefficient (d33) value of 3.5 pC N−1 for its pellet. The piezoelectric energy harvesting applications on the sandwich devices fabricated from the as‐made crystals of RMBA‐BF3 gave an open circuit voltage (VPP) of 6.2 V. This work thus underscores the untapped potential of B−N adducts in the field of piezoelectric energy harvesting.

Funder

Science and Engineering Research Board

University of Hyderabad

Laboratorio Nacional de Supercómputo del Sureste de Mexico

Publisher

Wiley

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