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Symmetric Mass Generation with four SU(2) doublet fermions

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arxiv 2409.02062 v2 pith:JO42JJLQ submitted 2024-09-03 hep-lat hep-phhep-th

classification hep-lathep-phhep-th
keywords phaseconformalcouplingfermiongaugegenerationmassstrong
verification ladder T0 review T1 audit T2 compute T3 formal
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abstract

We study a single exactly massless staggered fermion in the fundamental representation of an $SU(2)$ gauge group. We utilize an nHYP-smeared fermion action supplemented with additional heavy Pauli-Villars fields which serve to decrease lattice artifacts. The phase diagram exhibits a clear two-phase structure with a conformal phase at weak coupling and a novel new phase, the Symmetric Mass Generation (SMG) phase, appearing at strong coupling. The SMG phase is confining with all states gapped and chiral symmetry unbroken. Our finite size scaling analysis provides strong evidence that the phase transition between these two phases is continuous, which would allow for the existence of a continuum SMG phase. Furthermore, the RG flows are consistent with a $\beta$-function that vanishes quadratically at the new fixed point suggesting that the $N_f=4$ flavor SU(2) gauge theory lies at the opening of the conformal window.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Investigating SU(3) with Nf=8 fundamental fermions at strong renormalized coupling

    hep-lat 2024-12 conditional novelty 6.0 of 10

    Finite-size scaling of lattice data favors a merged fixed point governing the strong-to-weak coupling transition in SU(3) with eight fundamental flavors, suggesting this system sits at the opening of the conformal window.

  2. Scale Separation, Strong Coupling UV Phases, and the Identification of the Edge of the Conformal Window

    hep-ph 2024-12 conditional novelty 6.0 of 10

    A holographic model shows that near the conformal window edge, chiral symmetry breaking can be hidden by scale separation and by a UV artefact phase, making lattice phase identification hard, though the Nf=10 SU(3) re...

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