Epstein Secrets

t of =11 trajectories along which this information can flow, as seen from the pe=spective of an observer. We can get such an arrangement from a flat lattic= (i.e. a graph) that is approximately regular and fine grained enough. If =e disturb the lattice structure by adding more links, we get nonlocality (

lculat= more than a Turing machine. However, that conflicts with the traditional =ntuitions of most of physics: that the universe is geometric, i.e. hyperco=putational. The fact that we cannot construct a hypercomputer, not just no= in physics, but also not mathematically (where we take its existence as g

t of =11 trajectories along which this information can flow, as seen from the pe=spective of an observer. We can get such an arrangement from a flat lattic= (i.e. a graph) that is approximately regular and fine grained enough. If =e disturb the lattice structure by adding more links, we get nonlocality (

lculat= more than a Turing machine. However, that conflicts with the traditional =ntuitions of most of physics: that the universe is geometric, i.e. hyperco=putational. The fact that we cannot construct a hypercomputer, not just no= in physics, but also not mathematically (where we take its existence as g

t of =11 trajectories along which this information can flow, as seen from the pe=spective of an observer. We can get such an arrangement from a flat lattic= (i.e. a graph) that is approximately regular and fine grained enough. If =e disturb the lattice structure by adding more links, we get nonlocality (

lculat= more than a Turing machine. However, that conflicts with the traditional =ntuitions of most of physics: that the universe is geometric, i.e. hyperco=putational. The fact that we cannot construct a hypercomputer, not just no= in physics, but also not mathematically (where we take its existence as g