Cobordism and Deformation Class of the Standard Model

Understand

't Hooft anomalies of quantum field theories (QFTs) with an invertible global symmetry G (including spacetime and internal symmetries) in a $d$d spacetime are known to be classified by a $d+1$d cobordism group TP$_{d+1}$(G), whose group generator is a $d+1$d cobordism invariant written as an invertible topological field theory (iTFT) Z$_{d+1}$.

• The deformation class of QFT is recently proposed to be specified by its symmetry G and an iTFT Z$_{d+1}$.
• Seemingly different QFTs of the same deformation class can be deformed to each other via quantum phase transitions.
• In this work, we ask which deformation class controls the 4d ungauged or gauged (SU(3)$\times$SU(2)$\times$U(1))/$\mathbb{Z}_q$ Standard Model (SM) for $q=1,2,3,6$ with a continuous or discrete $(\bf{B}-\bf{L})$ symmetry.