its a q all over the net in physics Nimit
Here is a sample and link to the blogs, not further on where to find Hans for further view.
"Big bang of a particle and the creation of worlds
Say, you are master of the LHC. During an experiment you create a single particle that combines all symmetries contained in E8, but also all corresponding anti-symmetries. You ensure that all fields that act on symmetries are present and are sufficiently strong. In that case the particle will spontaneously and enforced break down and the pieces will all take their own paths.
Let |f> be that particle at time t0. t0 is the time of the explosion. The result will be a series of parts with states |fn> that each have a characteristic set of symmetries or anti-symmetries. If time is reversed the explosion will become an implosion and we observe a new set of particles that behave differently with respect to the first set. Call the new particles fundamental particles. Now give each of these sub-particles their own Hilbert space. Each Hilbert space has its own scaling, its own time direction and its own calculation rules. Call this a tensor division of the original Hilbert space that described the conglomerate. Bosons have symmetric density distribution over space. Fermions have an anti-symmetric density distribution over space.
Now a superman can create a new world by constructing a tensor product of two or more Hilbert spaces of the fundamental particles. The origin of the quaternion fields of the spacetime observables in the different Hilbert spaces can be taken at different locations. The (re)combination has to be done according to certain rules. It can be done more careless with bosons than with fermions. With identical fermions the order of the combination is relevant. Identical fermions cannot take the same positions. The result is the Hilbert space of the corresponding world.
Hans"
https://www.researchgate.net/group/N...c=22578#c22578
kind regards graham


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