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    Spectroscopic Demarcation of Emergent Photons and Spinons in a Dipolar-Octupolar Quantum Spin Liquid

    Bin Gao1,2,*, Zhengbang Zhou3,*, Tingjun Zhang1,2,4, Andrey Podlesnyak5, Sang-Wook Cheong6, Yong Baek Kim3,†, and Pengcheng Dai1,2,‡

    • 1Department of Physics and Astronomy, Rice University, Houston, Texas 77005, USA
    • 2Rice Laboratory for Emergent Magnetic Materials and Smalley-Curl Institute, Rice University, Houston, Texas 77005, USA
    • 3Department of Physics, University of Toronto, Toronto, Ontario M5S 1A7, Canada
    • 4Applied Physics Graduate Program, Smalley-Curl Institute, Rice University, Houston, Texas 77005, USA
    • 5Neutron Scattering Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
    • 6Keck Center for Quantum Magnetism and Department of Physics and Astronomy, Rutgers University, Piscataway, New Jersey 08854, USA

    • *These authors contributed equally to this work.
    • †Contact author: yongbaek.kim@utoronto.ca
    • ‡Contact author: pdai@rice.edu

    Phys. Rev. Lett. 136, 256703 – Published 23 June, 2026

    DOI: https://doi.org/10.1103/svt2-m3pp

    Abstract

    The identification of fractionalized excitations in quantum spin liquids (QSLs) remains a central challenge in condensed matter physics. In dipolar-octupolar (DO) pyrochlores, such as Ce2Zr2O7, the candidate π-flux quantum spin ice (QSI) state is predicted to host both gapless emergent photons and a continuum of spinons. However, resolving these modes at zero field is complicated by their spectral overlap and the presence of nonmagnetic scattering near zero energy. Here, we report neutron scattering experiments on Ce2Zr2O7 under a magnetic field along the [1, 1, 1] direction. In contrast to previous unpolarized studies at zero field that relied on high-temperature subtraction, we use a same-temperature high-field subtraction protocol to isolate the photon and spinon modes. Leveraging the selective coupling of the magnetic field to the dipolar degrees of freedom, we demonstrate the spectroscopic demarcation of these excitations. We observe that weak fields (≈0.15  T) suppress the low-energy photon weight while leaving the high-energy spinon continuum robust, albeit hardened. Our results, supported by gauge mean-field theory and exact diagonalization calculations, provide strong evidence for the π-flux QSI state and introduce a powerful field-tuning protocol for investigating DO-QSLs.

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