Nonresonant Raman Control of Ferroelectric Polarization

J Jiaojian Shi (Department of Materials Science and Engineering Stanford University Stanford CA 94305 USA) C Christian Heide H Haowei Xu Y Yuejun Shen (Department of Materials Science and Engineering Stanford University Stanford CA 94305 USA) M Meredith Henstridge (Laser Science and Technology SLAC Linear Accelerator Laboratory Menlo Park CA 94025 USA) I Isabel Sedwick (Department of Chemistry University of Washington Seattle WA 98195 USA) A Anudeep Mangu (Department of Materials Science and Engineering, Stanford University) X Xinyue Peng S Shangjie Zhang (Department of Physics, Center for Complex Quantum Systems The University of Texas at Austin Austin TX 78712 USA) M Mariano Trigo (Stanford PULSE Institute, SLAC National Accelerator Laboratory 6 , Menlo Park, California 94025,) T Tony F. Heinz J Ju Li K Keith A. Nelson E Edoardo Baldini (Department of Physics) J Jian Zhou S Shambhu Ghimire (Stanford PULSE Institute SLAC National Accelerator Laboratory Menlo Park CA 94025 USA) D David A. Reis (Stanford PULSE Institute, SLAC National Accelerator Laboratory 6 , Menlo Park, California 94025,) A Aaron M. Lindenberg

Abstract

Abstract Important advances is recently made in the search for materials with complex multi‐phase landscapes that host photoinduced metastable collective states with exotic functionalities. In almost all cases so far, the desired phases are accessed by exploiting light–matter interactions via the imaginary part of the dielectric function through above‐bandgap or resonant mode excitation. Nonresonant Raman excitation of coherent modes is experimentally observed and proposed for dynamic material control, but the resulting atomic excursion is limited to perturbative levels. Here, this challenge is overcome by employing nonresonant ultrashort pulses with low photon energies well below the bandgap. Using mid‐infrared pulses, ferroelectric reversal is induced in lithium niobate, and the large‐amplitude mode displacements are characterized through femtosecond stimulated Raman scattering and second harmonic generation. This approach, validated by first‐principle calculations, defines a novel method for synthesizing hidden phases with unique functional properties and manipulating complex energy landscapes at reduced energy consumption and ultrafast speeds.

Article Details

Volume / Issue Vol. 37, Issue 44
Published November 01, 2025
ISSN 0935-9648
Publisher Unknown Publisher

Journal Info

Advanced Materials

Unknown Publisher

ISSN: 0935-9648 Physical Sciences

Authors (18)

J

Jiaojian Shi

Department of Materials Science and Engineering Stanford University Stanford CA 94305 USA

C

Christian Heide

H

Haowei Xu

Y

Yuejun Shen

Department of Materials Science and Engineering Stanford University Stanford CA 94305 USA

M

Meredith Henstridge

Laser Science and Technology SLAC Linear Accelerator Laboratory Menlo Park CA 94025 USA

I

Isabel Sedwick

Department of Chemistry University of Washington Seattle WA 98195 USA

A

Anudeep Mangu

Department of Materials Science and Engineering, Stanford University

X

Xinyue Peng

S

Shangjie Zhang

Department of Physics, Center for Complex Quantum Systems The University of Texas at Austin Austin TX 78712 USA

M

Mariano Trigo

Stanford PULSE Institute, SLAC National Accelerator Laboratory 6 , Menlo Park, California 94025,

T

Tony F. Heinz

J

Ju Li

K

Keith A. Nelson

E

Edoardo Baldini

Department of Physics

J

Jian Zhou

S

Shambhu Ghimire

Stanford PULSE Institute SLAC National Accelerator Laboratory Menlo Park CA 94025 USA

D

David A. Reis

Stanford PULSE Institute, SLAC National Accelerator Laboratory 6 , Menlo Park, California 94025,

A

Aaron M. Lindenberg