Abstract

We study SU(Nc) gauge theories with Dirac fermions in representations ℛ of nonzero N -ality, coupled to axions. These theories have an exact discrete chiral symmetry, which has a mixed ’t Hooft anomaly with general baryon-color-flavor backgrounds, called the “BCF anomaly” in [1]. The infrared theory also has an emergent {mathrm{mathbb{Z}}}_{N_c}^{(1)} 1-form center symmetry. We show that the BCF anomaly is matched in the infrared by axion domain walls. We argue that {mathrm{mathbb{Z}}}_{N_c}^{(1)} is spontaneously broken on axion domain walls, so that nonzero N -ality Wilson loops obey the perimeter law and probe quarks are deconfined on the walls. We give further support to our conclusion by using a calculable small-circle compactification to study the multi-scale structure of the axion domain walls and the microscopic physics of deconfinement on their worldvolume.

Highlights

  • We study SU(Nc) gauge theories with Dirac fermions in representations R of nonzero N -ality, coupled to axions

  • We show that the BCF anomaly is matched in the infrared by axion domain walls

  • We show that the deconfinement and rearrangement of heavy degrees of freedom on the axion domain wall are intertwined

Read more

Summary

We argue that

N -ality Wilson loops obey the perimeter law and probe quarks are deconfined on the walls. We give further support to our conclusion by using a calculable small-circle compactification to study the multi-scale structure of the axion domain walls and the microscopic physics of deconfinement on their worldvolume. Elucidating the microscopic nature of the worldvolume physics is the main goal of this paper This is not straightforward on R4, as the physics determining the domain wall behavior is not semiclassically accessible, contrary to naive expectations — despite the axion’s lightness, axion domain walls probe the much shorter distance scales of order the confinement scale, representing a subtle failure of effective field theory (EFT) that has been anticipated earlier.

We take the
The potential in is
LT QF T
9In addition to the possible
As is the case on
To leading exponential accuracy in the v
These are at σq
ZNc action maps σq to σq
Nf TR Nc
They correspond with q and q
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call