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188宝金博页面版: tensionless branes and the null string critical dimension

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内容提示: arXiv:hep-th/9711136v2 6 Apr 1998hep-th/9711136JINR-E2-98-84TENSIONLESS BRANES AND THE NULL STRING CRITICALDIMENSION1P. Bozhilov2Bogoliubov Laboratory of Theoretical Physics, JINR, Dubna, RussiaE-mail: bojilov@thsun1.jinr.dubna.suBRST quantization is carried out for a model of p-branes with second class constraints.After extension of the phase space the constraint algebra coincides with the one of null stringwhen p = 1. It is shown that in this case one can or can not obtain critical dimension forthe null...

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arXiv:hep-th/9711136v2 6 Apr 1998hep-th/9711136JINR-E2-98-84TENSIONLESS BRANES AND THE NULL STRING CRITICALDIMENSION1P. Bozhilov2Bogoliubov Laboratory of Theoretical Physics, JINR, Dubna, RussiaE-mail: bojilov@thsun1.jinr.dubna.suBRST quantization is carried out for a model of p-branes with second class constraints.After extension of the phase space the constraint algebra coincides with the one of null stringwhen p = 1. It is shown that in this case one can or can not obtain critical dimension forthe null string, depending on the choice of the operator ordering and corresponding vacuumstates. When p > 1, operator orderings leading to critical dimension in the p = 1 case arenot allowed. Admissable orderings give no restrictions on the dimension of the embeddingspace-time. Finally, a generalization to supersymmetric null branes is proposed.1Work supported in part by the National Science Foundation of Bulgaria under contract φ − 620/19962permanent address: Dept.of Theoretical Physics,”Konstantin Preslavsky” Univ. of Shoumen9700 Shoumen, Bulgaria E-mail: bojilov@uni-shoumen.bg

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