Bell's spaceship paradox: Difference between revisions

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{{Unreferenced|auto=yes|date=December 2009}}
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In [[theoretical physics]] '''Pohlmeyer charge''', named for [[:de:Klaus Pohlmeyer|Klaus Pohlmeyer]], is a conserved [[Charge invariance|charge invariant]] under the [[Virasoro algebra]] or its generalization. It can be obtained by expanding the [[holonomy|holonomies]] (generating functions)
 
:<math>P\,Tr\, \exp i T_\mu\oint d\sigma A_\sigma^{(\mu)}(\sigma)</math>
 
with respect to the constant matrices ''T''. The gauge field <math>A_\sigma^\mu</math> is defined as a combination of <math>\partial X^\mu</math> and its conjugate.
 
According to the logic of [[loop quantum gravity]] and [[algebraic quantum field theory]], these charges are the right physical quantities that should be used for quantization. This logic is however incompatible with the standard and well-established methods of [[quantum field theory]] based on [[Fock space]] and [[perturbation theory]].
 
 
 
[[Category:Theoretical physics]]
 
{{DEFAULTSORT:Pohlmeyer Charge}}
 
 
{{Phys-stub}}

Latest revision as of 23:24, 30 June 2014

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