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bapowell
Science Advisor
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I refuse to engage in this ridiculous discussion regarding things not being nothings and no nothings can't be a something because a nothing is nothing and so can't possibly be a something. I will, however, gladly talk about physics, since that's what this forum is all about.apeiron said:Can you explain how a supersymmetric vacuum is actually not still a something? It seems to be a scalar field of energy in suspension at least.
In quantum field theory, the vacuum fluctuations of bosons and fermions contribute to the ground state energy with different signs. This is a consequence of the spin-statistics theorem: bosons give a positive contribution, and fermions a negative one. In a supersymmetric theory, each fermion has a bosonic partner of equal mass. Therefore, the fluctuations of each species cancel to all orders in perturbation theory. The result: the vacuum of a supersymmetric theory has zero energy.
As far as I know, supersymmetry is not broken by any sort of fluctuation. Can you elaborate on what you mean here? SUSY, like most other symmetries in particle physics, are broken when some field in theory assumes a nonzero expectation value (the symmetry is governed by a scalar order parameter, much like in condensed matter systems). Again, not sure what you mean by 'how large' the vacuum is. Of course, our observable universe isn't supersymmetric. However, there may be other vacua (ie other places in the universe) that may well be supersymmetric.And what are the rules about the fluctuations that can spontaneously break its symmetry. How large is this vacuum and in how many places at how many times can it be broken?