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Deformations and spectral properties of merons
We consider a meron–antimeron pair located at a, b, ∈ R4, and show that the spectrum of its stability operator is not bounded below [in precise mathematical terms: The stability operator defined on C ∞ 0(R4−{a,b}) has a self‐adjoint extension, possibly many, all of which are unbounded below]. We reg...
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Published in: | Journal of mathematical physics 1979-10, Vol.20 (10), p.2097-2109 |
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Main Author: | |
Format: | Article |
Language: | English |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | We consider a meron–antimeron pair located at a, b, ∈ R4, and show that the spectrum of its stability operator is not bounded below [in precise mathematical terms: The stability operator defined on C
∞
0(R4−{a,b}) has a self‐adjoint extension, possibly many, all of which are unbounded below]. We regularize a single meron located at the origin by replacing it inside a sphere of radius R
0 and outside a sphere of radius R by ’’half instantons,’’ and show that for R≫R
0 the regularized configuration continues to be unstable. For R
0 finite and R=∞, we show that the spectrum of the stability operator continues to extend to −∞. We employ a singular transformation to embed R4 into S
3×R where the meron pair takes a simple form and its stability operator L becomes L=−d
2/dτ2+V, where τ∈R, and the potential V can be diagonalized in terms of the angular momenta, spin, and isospin of the vector field. The spectrum of L is continuous and extends from −2 to +∞. We determine the number of (generalized) zero eigenmodes of L, and calculate its spectrum explicitly. |
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ISSN: | 0022-2488 1089-7658 |
DOI: | 10.1063/1.523978 |