Answers are grounded in this paper and cite their sources.
Storage rings that hold a beam's spin frozen relative to its momentum — built to search for electric dipole moments — are, by construction, exquisitely sensitive to any additional spin precession, including the precession an axial torsion background would drive. This paper converts their design sensitivities into torsion bounds. A proton frozen-spin ring targeting a precession sensitivity of 1e-09 radians per second bounds an axial torsion background at 3.34e-18 per metre, equivalent to a spin energy of 6.58e-25 eV; a deuteron ring at an existing facility, at 1e-07 radians per second, bounds it at 3.34e-16 per metre. The proton-ring figure is the second-strongest background-torsion bound in the laboratory, behind only comagnetometers, and it is obtained with a completely different systematic profile: a circulating relativistic beam rather than a stationary vapour. The paper also computes the torsion the ring's own polarised beam sources for itself — 3.28e-54 per metre for 1e11 polarised protons in a bunch — thirty-six orders below the bound, so self-sourcing is no correction at any foreseeable sensitivity. Two caveats are stated plainly: a torsion precession in a single ring is degenerate with an electric dipole signal, and the bound applies to backgrounds and extensions, since the minimal Einstein-Cartan theory provides no torsion in the ring's vacuum. Computed from stated assumptions, not measured.
No takes yet. Share an insight, caveat, or question.
William Alexander Aldred (2026) studied this question.
Synapse has enriched 8 closely related papers on similar clinical questions. Consider them for comparative context: