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arxiv: 1208.6214 · v2 · pith:IOCNSDEBnew · submitted 2012-08-30 · ❄️ cond-mat.str-el · cond-mat.quant-gas· nucl-th

Efimov effect in quantum magnets

classification ❄️ cond-mat.str-el cond-mat.quant-gasnucl-th
keywords efimoveffectmagnetsmagnonsphysicsquantumuniversalstates
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Physics is said to be universal when it emerges regardless of the underlying microscopic details. A prominent example is the Efimov effect, which predicts the emergence of an infinite tower of three-body bound states obeying discrete scale invariance when the particles interact resonantly. Because of its universality and peculiarity, the Efimov effect has been the subject of extensive research in chemical, atomic, nuclear and particle physics for decades. Here we employ an anisotropic Heisenberg model to show that collective excitations in quantum magnets (magnons) also exhibit the Efimov effect. We locate anisotropy-induced two-magnon resonances, compute binding energies of three magnons and find that they fit into the universal scaling law. We propose several approaches to experimentally realize the Efimov effect in quantum magnets, where the emergent Efimov states of magnons can be observed with commonly used spectroscopic measurements. Our study thus opens up new avenues for universal few-body physics in condensed matter systems.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Universal Bound States in Long-range Spin Chains with an Impurity

    quant-ph 2025-07 unverdicted novelty 7.0

    Resonant two-magnon interactions in long-range spin chains yield Efimov three-magnon states for alpha in (2, 2.89) and semi-super Efimov states at alpha=2, confirmed by numerical solution of the Skorniakov-Ter-Martiro...

  2. Efimov Effect in Long-range Quantum Spin Chains

    cond-mat.quant-gas 2025-02 unverdicted novelty 7.0

    Long-range interactions in quantum spin chains enable the Efimov effect for magnons by inducing continuous scale invariance in two-body states that becomes discrete in the three-body problem.