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This study utilizes advanced tensor-network methods to compute the dynamical spectral function of the $J_1$-$J_2$ kagome Heisenberg model, successfully characterizing it as a U(1) Dirac spin liquid. By tracking excitation evolution across magnetic phases, researchers have identified specific spectral fingerprints for deconfined spinons that could guide future experimental verification in candidate materials. The work provides critical theoretical benchmarks for understanding exotic fractionalized excitations in highly frustrated quantum magnets without relying on static order parameters.
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Dynamical Spectral Function of the Kagome Quantum Spin Liquid

arXiv2 min de cititArticolul și perspectiva sunt în engleză.

arXiv:2512.18831v3 Announce Type: replace-cross Abstract: Quantum spin liquids (QSLs) host exotic fractionalized magnetic and gauge-field excitations whose microscopic origins and experimental verification remain frustratingly elusive. In the absence of static magnetic order, the spin excitation spectrum constitutes the crucial probe of QSL behavior, but its theoretical computation is a serious challenge. Here we employ state-of-the-art tensor-network methods to obtain the full dynamical spectral function of the $J_1$-$J_2$ kagome Heisenberg model and benchmark our results by tracking their evolution across the magnetically ordered and QSL phases. Reducing $|J_2|/J_1$ causes increasingly strong spin-wave renormalization, flattening these modes then merging them into a continuum characteristic of deconfined spinons at all finite energies in the QSL. The low-energy continuum and the occurrence of gap closure at multiple high-symmetry points identify this gapless QSL as the U(1) Dirac spin liquid. These results establish a unified understanding of spin excitations in highly frustrated quantum magnets and provide clear spectral fingerprints for experimental detection in candidate kagome QSL materials.

Abstract:Quantum spin liquids (QSLs) host exotic fractionalized magnetic and gauge-field excitations whose microscopic origins and experimental verification remain frustratingly elusive. In the absence of static magnetic order, the spin excitation spectrum constitutes the crucial probe of QSL behavior, but its theoretical computation is a serious challenge. Here we employ state-of-the-art tensor-network methods to obtain the full dynamical spectral function of the $J_1$-$J_2$ kagome Heisenberg model and benchmark our results by tracking their evolution across the magnetically ordered and QSL phases. Reducing $|J_2|/J_1$ causes increasingly strong spin-wave renormalization, flattening these modes then merging them into a continuum characteristic of deconfined spinons at all finite energies in the QSL. The low-energy continuum and the occurrence of gap closure at multiple high-symmetry points identify this gapless QSL as the U(1) Dirac spin liquid. These results establish a unified understanding of spin excitations in highly frustrated quantum magnets and provide clear spectral fingerprints for experimental detection in candidate kagome QSL materials.

Strongly Correlated Electrons (cond-mat.str-el); Quantum Physics (quant-ph)

arXiv:2512.18831 [cond-mat.str-el]

(or arXiv:2512.18831v3 [cond-mat.str-el] for this version)

https://doi.org/10.48550/arXiv.2512.18831 Focus to learn more arXiv-issued DOI via DataCite

Phys. Rev. Lett. 137, 076504 (2026)

https://doi.org/10.1103/fjjf-xspp Focus to learn more DOI(s) linking to related resources

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