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arxiv: 0808.3965 · v2 · submitted 2008-08-28 · ✦ hep-ph · hep-lat· nucl-th

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Hadrons in Strong Electric and Magnetic Fields

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classification ✦ hep-ph hep-latnucl-th
keywords fieldselectricmagneticstrongchiralnucleonsperturbationperturbative
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We use chiral perturbation theory to investigate hadronic properties in strong electric and magnetic fields. A strong-field power counting is employed, and results for pions and nucleons are obtained using Schwinger's proper-time method. In the limit of weak fields, we accordingly recover the well known one-loop chiral perturbation theory results for the electric and magnetic polarizabilities of pions and nucleons. In strong constant fields, we extend the Gell-Mann-Oakes-Renner relation. For the case of electric fields, we find that non-perturbative effects result in hadron decay. For sufficiently strong magnetic fields, the chiral analysis confirms that the nucleon hierarchy becomes inverted giving rise to proton beta-decay. Properties of asymptotic expansions are explored by considering weak field limits. In the regime where the perturbative expansion breaks down, the first-order term gives the best agreement with the non perturbative result.

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  1. Charged kaon electric polarizability from four-point functions in lattice QCD

    hep-lat 2026-04 unverdicted novelty 6.0

    Lattice QCD on quenched 24^3 x 48 lattices yields charged kaon electric polarizability α_E = (0.988 ± 0.534) × 10^{-4} fm³ and charge radius squared 0.3303 ± 0.0028 fm² after physical pion-mass extrapolation.