TY - JOUR
T1 - Phase Diagram of the Two-Flavor Schwinger Model at Zero Temperature
AU - Dempsey, Ross
AU - Klebanov, Igor R.
AU - Pufu, Silviu S.
AU - Søgaard, Benjamin T.
AU - Zan, Bernardo
N1 - Publisher Copyright:
© 2024 authors. Published by the American Physical Society. Published by the American Physical Society under the terms of the "https://creativecommons.org/licenses/by/4.0/"Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article's title, journal citation, and DOI. Funded by SCOAP
PY - 2024/1/19
Y1 - 2024/1/19
N2 - We examine the phase structure of the two-flavor Schwinger model as a function of the θ angle and the two masses, m1 and m2. In particular, we find interesting effects at θ=π: along the SU(2)-invariant line m1=m2=m, in the regime where m is much smaller than the charge g, the theory undergoes logarithmic renormalization group flow of the Berezinskii-Kosterlitz-Thouless type. As a result, dimensional transmutation takes place, leading to a nonperturbatively small mass gap ∼e-Ag2/m2. The SU(2)-invariant line lies within a region of the phase diagram where the charge conjugation symmetry is spontaneously broken and whose boundaries we determine numerically. Our numerical results are obtained using the Hamiltonian lattice gauge formulation that includes the mass shift mlat=m-g2a/4 dictated by the discrete chiral symmetry.
AB - We examine the phase structure of the two-flavor Schwinger model as a function of the θ angle and the two masses, m1 and m2. In particular, we find interesting effects at θ=π: along the SU(2)-invariant line m1=m2=m, in the regime where m is much smaller than the charge g, the theory undergoes logarithmic renormalization group flow of the Berezinskii-Kosterlitz-Thouless type. As a result, dimensional transmutation takes place, leading to a nonperturbatively small mass gap ∼e-Ag2/m2. The SU(2)-invariant line lies within a region of the phase diagram where the charge conjugation symmetry is spontaneously broken and whose boundaries we determine numerically. Our numerical results are obtained using the Hamiltonian lattice gauge formulation that includes the mass shift mlat=m-g2a/4 dictated by the discrete chiral symmetry.
UR - http://www.scopus.com/inward/record.url?scp=85183031022&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=85183031022&partnerID=8YFLogxK
U2 - 10.1103/PhysRevLett.132.031603
DO - 10.1103/PhysRevLett.132.031603
M3 - Article
C2 - 38307058
AN - SCOPUS:85183031022
SN - 0031-9007
VL - 132
JO - Physical review letters
JF - Physical review letters
IS - 3
M1 - 031603
ER -