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Nucleon electric polarizabilities and nucleon-pion scattering at physical pion mass

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arxiv 2310.01168 v3 pith:3TRKTJAP submitted 2023-10-02 hep-lat hep-exhep-phnucl-ex

classification hep-lathep-exhep-phnucl-ex
keywords latticepolarizabilitiescontributionsnucleonelectricmassphysicalpion
verification ladder T0 review T1 audit T2 compute T3 formal

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abstract

We present a lattice QCD calculation of the nucleon electric polarizabilities at the physical pion mass. Our findings reveal the substantial contributions of the $N\pi$ states to these polarizabilities. Without considering these contributions, the lattice results fall significantly below the experimental values, consistent with previous lattice studies. This observation has motivated us to compute both the parity-negative $N\pi$ scattering up to a nucleon momentum of $\sim0.5$ GeV in the center-of-mass frame and corresponding $N\gamma^*\to N\pi$ matrix elements using lattice QCD. Our results confirm that incorporating dynamic $N\pi$ contributions is crucial for a reliable determination of the polarizabilities from lattice QCD. This methodology lays the groundwork for future lattice QCD investigations into various other polarizabilities.

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Cited by 3 Pith papers

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    A new stochastic estimator, blending distillation low modes with reweighted random high modes, gives unbiased all-to-all fermion propagators and enables sub-percent nucleon axial charge and 4-point pion form factor ca...

  2. The Neutron Electric Dipole Moment from Lattice QCD using a Background Electric Field

    hep-lat 2026-07 conditional novelty 7.0 of 10

    Using background electric fields, local topological charge, and non-Hermitian GEVP, lattice QCD yields dn = -0.0050(4)stat(8)sys θ-bar e fm at the physical point.

  3. Electromagnetic polarizabilities of the spin-$\frac{1}{2}$ singly heavy baryons in heavy baryon chiral perturbation theory

    hep-ph 2024-12 conditional novelty 6.0 of 10

    At O(p^3) in heavy baryon chiral perturbation theory, sextet heavy baryons acquire polarizabilities from pion/kaon loops and from B6* to B6 magnetic transitions, while antitriplet heavy baryons have zero polarizability.

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