Bell's spaceship paradox: Difference between revisions

Revision as of 14:32, 15 February 2014

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-{{Unreferenced|auto=yes|date=December 2009}}
+I would like to introduce myself to you, I am Andrew and my spouse doesn't like it at all. To climb is some thing she would never give up. My wife and I live in Mississippi and I adore each working day living here. Invoicing is my occupation.<br><br>Feel free to visit my web site - free psychic ([http://c045.danah.co.kr/home/index.php?document_srl=1356970&mid=qna http://c045.danah.co.kr/])
-{{Orphan|date=February 2009}}
-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}}

Bell's spaceship paradox: Difference between revisions

Revision as of 14:32, 15 February 2014

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