Issue of choosing nothing: What Determines the low energy Vacuum state of nature?

dc.contributor.authorPadmanabhan, T.
dc.contributor.authorChoudhury, T. Roy
dc.date.accessioned2012-03-03T13:33:39Z
dc.date.available2012-03-03T13:33:39Z
dc.date.issued2000-09-28
dc.description.abstractStarting from an (unknown) quantum gravitational model, one can invoke a sequence of approximations to progressively arrive at quantum field theory (QFT) in curved spacetime, QFT in flat spacetime, nonrelativistic quantum mechanics and newtonian mechanics. The more exact theory can put restrictions on the range of possibilities allowed for the approximate theory which are not derivable from the latter - an example being the symmetry restrictions on the wave function for a pair of electrons. We argue that the choice of vacuum state at low energies could be such a `relic' arising from combining the principles of quantum theory and general relativity, and demonstrate this result in a simple toy model. Our analysis suggests that the wave function of the universe, when it describes the large volume limit of the universe, dynamically selects a vacuum state for matter fields - which in turn defines the concept of particle in the low energy limit. The result also has the potential for providing a concrete quantum mechanical version of Mach's principle.en_US
dc.identifier.urihttp://hdl.handle.net/11007/196
dc.language.isoenen_US
dc.publisherWorld Scientific Publishing Companyen_US
dc.relation.ispartofseriesModern Physics Letters A;Vol. 15, No. 29, 2000
dc.subjectQuantum field theory (QFT)en_US
dc.subjectMach's principleen_US
dc.subjectEnergyen_US
dc.subjectSymmetry restrictionsen_US
dc.titleIssue of choosing nothing: What Determines the low energy Vacuum state of nature?en_US
dc.typeArticleen_US

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