of some preferred algebraic structure E that must be
preserved. The free operations follow as automorphisms of E, which in turn leads to natural notions of free states. This unifies so many different QRTs!
of some preferred algebraic structure E that must be
preserved. The free operations follow as automorphisms of E, which in turn leads to natural notions of free states. This unifies so many different QRTs!
of some preferred algebraic structure E that must be
preserved. The free operations follow as automorphisms of E, which in turn leads to natural notions of free states. This unifies so many different QRTs!
of some preferred algebraic structure E that must be
preserved. The free operations follow as automorphisms of E, which in turn leads to natural notions of free states. This unifies so many different QRTs!
I'll use the ocasion to share my related seminar doi.org/10.52843/cas... on our recent paper "Path Integrals from spacetime quantum actions" (doi.org/10.1016/j.ao...).
The topic? Unifying "Quantum time" and Feynman's approach
I'll use the ocasion to share my related seminar doi.org/10.52843/cas... on our recent paper "Path Integrals from spacetime quantum actions" (doi.org/10.1016/j.ao...).
The topic? Unifying "Quantum time" and Feynman's approach