# Fermion Number 1/2 of Sphalerons and Spectral Mirror Symmetry

## TL;DR

This paper rederives the half-integer fermion number of the electroweak sphaleron using spectral mirror symmetry, linking zero modes and spectral deficiencies to fundamental topological properties.

## Contribution

It introduces a novel spectral mirror symmetry approach to explain the fermion number of the sphaleron, extending previous zero mode analyses.

## Key findings

- Spectral mirror symmetry is established at the sphaleron.
- Fermionic zero mode remains invariant under the new symmetry.
- The fermion number 1/2 is derived from spectral deficiency and zero modes.

## Abstract

We present a rederivation of the baryon and lepton numbers $\frac{1}{2}$ of the $SU(2)_L$ S sphaleron of the standard electroweak theory based on spectral mirror symmetry. We explore the properties of a fermionic Hamiltonian under discrete transformations along a noncontractible loop of field configurations that passes through the sphaleron and whose endpoints are the vacuum. As is well known, CP transformation is not a symmetry of the system anywhere on the loop, except at the endpoints. By augmenting CP with a chirality transformation, we observe that the Dirac Hamiltonian is odd under the new transformation precisely at the sphaleron, and this ensures the mirror symmetry of the spectrum, including the continua. As a consistency check, we show that the fermionic zero mode presented by Ringwald in the sphaleron background is invariant under the new transformation. The spectral mirror symmetry which we establish here, together with the presence of the zero mode, are the two necessary conditions whence the fermion number $\frac{1}{2}$ of the sphaleron can be inferred using the reasoning presented by Jackiw and Rebbi or, equivalently, using the spectral deficiency $\frac{1}{2}$ of the Dirac sea. The relevance of this analysis to other solutions is also discussed.