Speaker
Chengcheng Liu
Description
We follow a quantum Kaluza-Klein formulation where we solve for the quantum Riemannian geometry on A = C∞(M) ⊗ M2(C) in terms of classical Riemannian geometry on M, the finite quantum geometry on M2(C) and gauge-field like cross term. We look at how scalar fields on the total space decompose into multiplets of fields in M differing in mass.