Constraints on Symmetry Preserving Gapped Phases from Coupling Constant Anomalies
Abstract: In this note, we will characterize constraints on the possible IR phases of a given QFT by anomalies in the space of coupling constants. We will give conditions under which a coupling constant anomaly cannot be matched by a continuous family of symmetry preserving gapped phases, in which case the theory is either gapless, or exhibits spontaneous symmetry breaking or a phase transition. We additionally demonstrate examples of theories with coupling constant anomalies which can be matched by a family of symmetry preserving gapped phases without a phase transition and comment on the interpretation of our results for the spontaneous breaking of "$(-1)$-form global symmetries."
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- Different choices of integral lift of B2∈H2(Xd;ℤN)subscript𝐵2superscript𝐻2subscript𝑋𝑑subscriptℤ𝑁B_{2}\in H^{2}(X_{d};{\mathbb{Z}}_{N})italic_B start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ∈ italic_H start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT ( italic_X start_POSTSUBSCRIPT italic_d end_POSTSUBSCRIPT ; blackboard_Z start_POSTSUBSCRIPT italic_N end_POSTSUBSCRIPT ) are related by ℬ2↦→ℬ2+2πΛ2{\cal B}_{2}\mapstochar\rightarrow{\cal B}_{2}+2\pi\Lambda_{2}caligraphic_B start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ↦ → caligraphic_B start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT + 2 italic_π roman_Λ start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT where Λ2∈H2(Xd;ℤ)subscriptΛ2superscript𝐻2subscript𝑋𝑑ℤ\Lambda_{2}\in H^{2}(X_{d};{\mathbb{Z}})roman_Λ start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ∈ italic_H start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT ( italic_X start_POSTSUBSCRIPT italic_d end_POSTSUBSCRIPT ; blackboard_Z ).
- Here we will only focus on ℤN(1)superscriptsubscriptℤ𝑁1{\mathbb{Z}}_{N}^{(1)}blackboard_Z start_POSTSUBSCRIPT italic_N end_POSTSUBSCRIPT start_POSTSUPERSCRIPT ( 1 ) end_POSTSUPERSCRIPT background for which B2∈H2(Xd;ℤN)subscript𝐵2superscript𝐻2subscript𝑋𝑑subscriptℤ𝑁B_{2}\in H^{2}(X_{d};{\mathbb{Z}}_{N})italic_B start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ∈ italic_H start_POSTSUPERSCRIPT 2 end_POSTSUPERSCRIPT ( italic_X start_POSTSUBSCRIPT italic_d end_POSTSUBSCRIPT ; blackboard_Z start_POSTSUBSCRIPT italic_N end_POSTSUBSCRIPT ) has an integral lift. In general, the fractional part of Chern characters can different when B2subscript𝐵2B_{2}italic_B start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT does not have an integer lift.
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