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From Bosonic Topological Transition to Symmetric Fermion Mass Generation
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From Bosonic Topological Transition to Symmetric Fermion Mass Generation
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The bosonic topological transition (BTT) is a quantum critical point between the bosonic symmetry protected topological phase and the trivial phase. In this work, we derive a description of this transition in terms of compact quantum electrodynamics (QED) with four fermion flavors ($N_f=4$). This allows us to describe the transition in a lattice model with the maximal microscopic symmetry: an internal SO(4) symmetry. Within a systematic renormalization group analysis, we identify the critical point with the desired O(4) emergent symmetry and all expected deformations. By lowering the microscopic symmetry we recover the previous $N_f=2$ non-compact QED description of the BTT. Finally, by merging two BTTs we recover a previously discussed theory of symmetric mass generation, as an SU(2) quantum chromodynamics-Higgs theory with $N_f=4$ flavors of SU(2) fundamental fermions and one SU(2) fundamental Higgs boson. This provides a consistency check on both theories.
Forward citations
Cited by 2 Pith papers
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Bosonization versus the Nielsen-Ninomiya theorem
In the 2D modified Villain model, bosonized chiral lattice fermion operators yield a doubler-free but non-local reconstructed Dirac operator, consistent with Nielsen-Ninomiya, while the microscopic theory remains ultr...
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Bosonization versus the Nielsen-Ninomiya theorem
The 2D modified Villain model's Weyl operators reproduce free Dirac correlations in the continuum, and their no-doubler Dirac kernel is non-local, showing exactly how bosonization evades the Nielsen-Ninomiya theorem.
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