Unrestricted Linear Stability of the Massless Skyrmion

Unrestricted Linear Stability of the Massless Skyrmion Description / Abstract This record contains the manuscript, exact rational profile data, and computer-assisted verification scripts proving unrestricted three-dimensional linear orbital stability for the degree-one massless $SU(2)$ Skyrmion. We establish nonnegativity and nondegeneracy, modulo three spatial translations and three internal isorotations, of the full three-dimensional static Hessian at the degree-one massless hedgehog solution. The static quadratic form is shown to be coercive in the homogeneous energy space $\dot{H}^1(\mathbb{R}^3; \mathfrak{su}(2))$ on the orthogonal complement of the six-dimensional symmetry kernel. Consequently, the relativistic linearized wave evolution is orbitally stable in $\dot{H}^1 \times L^2$ for arbitrary finite-energy three-dimensional perturbations, removing the corotational symmetry restriction of prior stability results. The proof decomposes perturbations across all grand-spin angular channels $K \ge 0$ into decoupled polar and axial parity sectors. The axial quadratic form is manifestly nonnegative for all $K \ge 1$, with its $K = 1$ kernel spanned by the three isorotations. The radial $K = 0$ sector uses the spectral nonnegativity theorem of Creek, Donninger, Schlag, and Snelson, extended to exclude homogeneous $\dot{H}^1$ zero resonances. In the coupled $K = 1$ polar sector, we construct an exact analytical matrix ground-state factorization into a nonnegative integral of squares using the translation Jacobi field and a vacuum-changing infinitesimal chiral Jacobi field. Because the chiral mode approaches a nonzero constant at infinity, it does not belong to $\dot{H}^1$, leaving translations as the unique physical kernel in $K = 1$. For all higher polar channels ($K \ge 2$), a scalar Liouville transformation reduces the quadratic form to a $2 \times 2$ comparison matrix $M_\Lambda(r)$ that increases monotonically with $\Lambda = K(K + 1)$ for $\Lambda \ge 6$. Using the published rigorous Chebyshev rational polynomial profile enclosure of Creek, Donninger, Schlag, and Snelson, a standard-library Python verifier executing 128-bit outward-rounded integer arithmetic across 8,192 closed boxes on the compactified radial domain certifies $M_\Lambda(r) \ge \frac{3}{64r^2} I$ over the entire half-line. Because the massless essential spectrum begins at zero, a compact weighted embedding $\dot{H}^1 \hookrightarrow L^2(W\,dx)$ using the $O(r^{-6})$ decay of the background weight upgrades channelwise nonnegativity and kernel identification to full homogeneous $\dot{H}^1$ coercivity.

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Publication Details

Journal
Zenodo (CERN European Organization for Nuclear Research)
Published
2026-11-08
DOI
https://doi.org/10.5281/zenodo.24047051
Primary Topic
Advanced Mathematical Physics Problems
Type
preprint
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preprint

Unrestricted Linear Stability of the Massless Skyrmion

Cohen Alexander
1 links
Zenodo (CERN European Organization for Nuclear Research)
Advanced Mathematical Physics Problems
preprint

Unrestricted Linear Stability of the Massless Skyrmion

Cohen Alexander
preprint en

Abstract

Unrestricted Linear Stability of the Massless Skyrmion Description / Abstract This record contains the manuscript, exact rational profile data, and computer-assisted verification scripts proving unrestricted three-dimensional linear orbital stability for the degree-one massless $SU(2)$ Skyrmion. We establish nonnegativity and nondegeneracy, modulo three spatial translations and three internal isorotations, of the full three-dimensional static Hessian at the degree-one massless hedgehog solution. The static quadratic form is shown to be coercive in the homogeneous energy space $\dot{H}^1(\mathbb{R}^3; \mathfrak{su}(2))$ on the orthogonal complement of the six-dimensional symmetry kernel. Consequently, the relativistic linearized wave evolution is orbitally stable in $\dot{H}^1 \times L^2$ for arbitrary finite-energy three-dimensional perturbations, removing the corotational symmetry restriction of prior stability results. The proof decomposes perturbations across all grand-spin angular channels $K \ge 0$ into decoupled polar and axial parity sectors. The axial quadratic form is manifestly nonnegative for all $K \ge 1$, with its $K = 1$ kernel spanned by the three isorotations. The radial $K = 0$ sector uses the spectral nonnegativity theorem of Creek, Donninger, Schlag, and Snelson, extended to exclude homogeneous $\dot{H}^1$ zero resonances. In the coupled $K = 1$ polar sector, we construct an exact analytical matrix ground-state factorization into a nonnegative integral of squares using the translation Jacobi field and a vacuum-changing infinitesimal chiral Jacobi field. Because the chiral mode approaches a nonzero constant at infinity, it does not belong to $\dot{H}^1$, leaving translations as the unique physical kernel in $K = 1$. For all higher polar channels ($K \ge 2$), a scalar Liouville transformation reduces the quadratic form to a $2 \times 2$ comparison matrix $M_\Lambda(r)$ that increases monotonically with $\Lambda = K(K + 1)$ for $\Lambda \ge 6$. Using the published rigorous Chebyshev rational polynomial profile enclosure of Creek, Donninger, Schlag, and Snelson, a standard-library Python verifier executing 128-bit outward-rounded integer arithmetic across 8,192 closed boxes on the compactified radial domain certifies $M_\Lambda(r) \ge \frac{3}{64r^2} I$ over the entire half-line. Because the massless essential spectrum begins at zero, a compact weighted embedding $\dot{H}^1 \hookrightarrow L^2(W\,dx)$ using the $O(r^{-6})$ decay of the background weight upgrades channelwise nonnegativity and kernel identification to full homogeneous $\dot{H}^1$ coercivity.

Zenodo (CERN European Organization for Nuclear Research)
Stanford University (US)
Advanced Mathematical Physics Problems
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