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    Coherent Spin Pumping Originated from Sub-Terahertz Néel Vector Dynamics in Easy Plane α−Fe2O3/Pt

    Gregory Fritjofson1, Junyu Tang2, Atul Regmi1, Jacob Hanson-Flores1, Justin Michel3, Fengyuan Yang3, Ran Cheng4,2, and Enrique Del Barco1,*

    • *Contact author: delbarco@ucf.edu

    Phys. Rev. Lett. 135, 216704 – Published 19 November, 2025

    DOI: https://doi.org/10.1103/zsd7-vbwg

    Abstract

    We present a thorough study of spin-to-charge current interconversion in bulk and thin films of (0001) α−Fe2O3/Pt heterostructures by means of all-optical polarization-controlled microwave excitation at subterahertz frequencies. Our results demonstrate that coherent spin pumping is generated through excitations of both the quasiferromagnetic and quasiantiferromagnetic (q-AFM) modes of antiferromagnetic resonance, provided that the corresponding selection rules are met for the relative orientation between the microwave magnetic field h→ac and the magnetic moment m→0 of the hematite. In particular, our results unambiguously show that while a microwave field with h→ac⊥m→0 pumps a net spin angular momentum from the quasiferromagnetic mode, spin pumping from the q-AFM mode is only enabled when h→ac||m→0, as expected from the selection rules imposed by the Néel vector dynamics. Our findings significantly advance current understanding of spin pumping in easy-plane antiferromagnets not only by claiming a substantial contribution from the Néel-vector dynamics of the q-AFM mode but also by experimentally determining the relative strength of the intra- and cross-sublattice components of the spin-mixing conductance, challenging recent reports where the absence of spin pumping from the q-AFM mode in hematite was interpreted as a complete cancellation between these two components. We also provide an explanation for the previously reported observations and show how the q-AFM spin pumping actually vanishes for thin films, which we speculate being either due to an increased level of inhomogeneities or to insufficient film thickness for the q-AFM mode to fully realize.

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