1997
DOI: 10.1016/s0370-2693(97)00380-8
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Tensionless p-branes with manifest conformal invariance

Abstract: The quantization of the tensionless p-brane is discussed. Inspection of the constraint algebra reveals that the central extensions for the p-branes have a simple form. Using a Hamiltonian BRST scheme we find that the quantization is consistent in any space-time dimension while the quantization of the conformal tensionless p-brane gives a critical dimension $d=2$.Comment: 14 pages, no figure

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Cited by 8 publications
(20 citation statements)
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“…Here we don't discuss more. 44 The spacetime index in the light-cone base: {µ} = {+, −, I} and I = 2, · · · , D − 1.…”
Section: Discussionmentioning
confidence: 99%
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“…Here we don't discuss more. 44 The spacetime index in the light-cone base: {µ} = {+, −, I} and I = 2, · · · , D − 1.…”
Section: Discussionmentioning
confidence: 99%
“…where the subscript R in the right-hand side indicates the reordering into R-order 10 . In light-cone 9 We can obtain the R-ordering from the normal ordering in the tensionless limit T → 0. In detail, the string ground state |0 T of a tensile string with a tension T is annihilated by positive modes of right-moving and left-moving oscillators, {αn, αn; n > 0}.…”
Section: Generatorsmentioning
confidence: 99%
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“…Finally, we pay attention to the fact that in every one of the p subalgebras (at fixed a) of the constraint algebra, one can obtain non-trivial central extension and consequently -critical dimension (see Appendix). For example, taking string − like or W eyl ordering, one derives D = 25 + p, which appears to be critical dimension for the tensile p-brane [17], [16]. However, the considered quantum dynamical system is described by the f ull constraint algebra, where only trivial central extensions are possible.…”
Section: Classical Theorymentioning
confidence: 99%