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    Electronic orbital angular momentum dynamics mediated by electron-chiral phonon interactions in helical chains

    Jiaqi Chen1, Hong Sun1, Ning Zhao1, Cong Yang2,3, Yimin Yao4, Jiyong Fu5, Jun Liu2,3,*, and Jun Zhou1,†

    • 1Phonon Engineering Research Center of Jiangsu Province, Center for Quantum Transport and Thermal Energy Science, Institute of Physics Frontiers and Interdisciplinary Sciences, School of Physics and Technology, Nanjing Normal University, Nanjing 210023, China
    • 2Department of Mechanical and Aerospace Engineering, North Carolina State University, Raleigh, North Carolina 27695, USA
    • 3Organic and Carbon Electronics Lab (ORaCEL), North Carolina State University, Raleigh, North Carolina 27695, USA
    • 4State Key Laboratory of Materials for Integrated Circuits, Shenzhen Institute of Advanced Electronic Materials, Shenzhen Institutes of Advanced Technology, Chinese Academy of Sciences, Shenzhen 518055, China
    • 5Department of Physics, Qufu Normal University, Qufu, Shandong 273165, China

    • *Contact author: jliu38@ncsu.edu
    • †Contact author: zhoujunzhou@njnu.edu.cn

    Phys. Rev. B 114, 094413 – Published 7 August, 2026

    DOI: https://doi.org/10.1103/c42k-r3mm

    Abstract

    The generation of electron orbital angular momentum (OAM) is the key for the field of orbitronics. Recently, the observation of orbital Seebeck effect [Y. Nabei et al., Nat. Phys. 22, 245 (2026)] shows that OAM can be generated by chiral phonons in materials with broken inversion symmetry. However, how electron-chiral phonon (ECP) interaction affects electric-field-induced electronic OAM dynamics remains unclear. In this work, we investigate ECP-mediated electronic OAM dynamics in a one-dimensional helical chain described by a Su-Schrieffer-Heeger model. The microscopic electronic OAM is defined from the operator L̂jel=r̂j×P̂j, while the main dynamical calculations employ a phonon OAM-based approximation whose validity is benchmarked against the microscopic electronic OAM. We show that, under the local-equilibrium-center definition and in the electron-phonon coupling regime used in the main calculations, this approximation captures the main dynamical features of electronic OAM. The slowly varying axial component is associated with an orbital-Edelstein-like electronic OAM polarization, whereas the transverse components mainly exhibit coherent precessional dynamics. We further find that chirality controls the sign and dynamical pattern of electronic OAM, while spin-orbit coupling is not the dominant channel for the ECP-driven electronic OAM dynamics in the present model.

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