Abstract

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 R0 and outside a sphere of radius R by ’’half instantons,’’ and show that for R≫R0 the regularized configuration continues to be unstable. For R0 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 S3×R where the meron pair takes a simple form and its stability operator ℒ becomes ℒ=−d2/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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