t Hooft anomalies of quantum field theories (QFTs) with an invertible global symmetry G (including spacetime and internal symmetries) in a dd spacetime are known to be classified by a d + 1d cobordism group TP d+1 (G), whose group generator is a d + 1d cobordism invariant written as an invertible topological field theory (iTFT) Z d+1 . Deformation class of QFT is recently proposed to be specified by its symmetry G and an iTFT Z d+1 . Seemly different QFTs of the same deformation class can be deformed to each other via quantum phase transitions. In this work, we ask which cobordism class and deformation class control the 4d Standard Model (SM) of ungauged or gauged (SU(3) × SU(2) × U(1))/Zq for q = 1, 2, 3, 6. We show that the answer contains some combination of 5d iTFTs: two Z classes associated with (B − L) 3 and (B − L)-(gravity) 2 4d perturbative local anomalies, a Z16 class Atiyah-Patodi-Singer η invariant and a Z2 class Stiefel-Whitney w2w3 invariant associated with 4d nonperturbative global anomalies, and additional Z4 × Z3 × Z2 classes involving higher symmetries whose charged objects are Wilson electric or 't Hooft magnetic line operators. Out of the multiple infinite Z classes of local anomalies and 24576 classes of global anomalies, we pin down a deformation class of SM labeled by (nν e,R , nν µ,R , nν τ,R , N f , p ′ , q), the "right-handed sterile" neutrino and family numbers, magnetic monopole datum, and mod q relation. We show that various Grand Unifications such as Georgi-Glashow su(5), Pati-Salam su(4) × su(2) × su(2), Barr's flipped u(5), and familiar or modified so(n) models of Spin(n) gauge group, e.g., with n = 10, 18 can all reside in an appropriate SM deformation class. We show that Ultra Unification, which replaces some of sterile neutrinos with new exotic gapped/gapless sectors (e.g., topological or conformal field theory) or gravitational sectors with topological origins via cobordism constraints, also resides in an SM deformation class. Neighbor quantum phases near SM or their phase transitions, and neighbor gapless quantum critical regions naturally exhibit beyond SM phenomena.