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This paper examines why singlet pairing in niobium suppresses the spin source for torsion even though the electron density is among the highest available in a solid. The system considered is niobium with a conduction-electron density near 5.6 x 10^28 per cubic metre, and the observable is pair density, singlet suppression and residual triplet torsion energy. Evaluating the ordinary behaviour of the system and the spin-torsion contribution under explicit assumptions about polarisation and uniformity, and inverting the comparison at the stated laboratory precision, gives a quantitative bound rather than a qualitative assertion of smallness. The computed record is: electron_density_per_m3 = 5.600e+28; pair_density_per_m3 = 2.800e+28; uT_if_fully_polarised_J_m3 = 3.885e-38; uT_singlet_J_m3 = 0; uT_triplet_1em3_J_m3 = 3.885e-44; gap_eV = 0.0015. The torsion-related contribution is far below the level that would alter the ordinary behaviour of the system at current precision, and the value that would have produced a visible residual is stated so that future improvements can be assessed against it directly. No new measurement is reported. This study is simulated and computed from stated assumptions, not measured.
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William Alexander Aldred (2026) studied this question.
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