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The Nuclear Central Force in the Chiral Limit

1 Pith paper cite this work. Polarity classification is still indexing.

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abstract

Chiral perturbation theory supplemented by the Omnes function is employed to study the strength of the isoscalar central nuclear interaction, G_S, in the chiral limit vs the physical case. A very large modification is seen, i.e. eta_s = G_S ~ chiral /G_S ~ physical = 1.37 +- 0.10 . This large effect is seen to arise dominantly at low energy from the extra contributions made by massless pions at energies near the physical threshold where the physical spectral function must vanish kinematically. The slope away from the chiral limit, d_S, is also calculated and is correspondingly large. I also explain why this large variation is to be expected.

fields

hep-ph 1

years

2024 1

verdicts

UNVERDICTED 1

representative citing papers

Weak nuclear decays deep-underground as a probe of axion dark matter

hep-ph · 2024-12-30 · unverdicted · novelty 6.0

A framework is developed to predict axion-induced time modulations in weak nuclear decays, used to derive constraints on the axion decay constant from reanalyzed Gran Sasso data on 40K and 137Cs and to propose future sensitivity to higher masses.

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Showing 1 of 1 citing paper.

  • Weak nuclear decays deep-underground as a probe of axion dark matter hep-ph · 2024-12-30 · unverdicted · none · ref 41 · internal anchor

    A framework is developed to predict axion-induced time modulations in weak nuclear decays, used to derive constraints on the axion decay constant from reanalyzed Gran Sasso data on 40K and 137Cs and to propose future sensitivity to higher masses.