Membrane duality revisited

被引:16
|
作者
Duff, M. J. [1 ]
Lu, J. X. [2 ]
Percacci, R. [3 ,4 ]
Pope, C. N. [5 ,6 ]
Samtleben, H. [7 ,8 ]
Sezgin, E. [5 ]
机构
[1] Univ London Imperial Coll Sci Technol & Med, Blackett Lab, Theoret Phys, London SW7 2AZ, England
[2] Univ Sci & Technol China, Interdisciplinary Ctr Theoret Study, Hefei 230026, Anhui, Peoples R China
[3] SISSA, I-34014 Trieste, Italy
[4] Ist Nazl Fis Nucl, Sez Trieste, Trieste, Italy
[5] Texas A&M Univ, George P & Cynthia W Mitchell Inst Fundamental Ph, College Stn, TX 77843 USA
[6] Univ Cambridge, Ctr Math Sci, DAMTP, Cambridge CB3 OWA, England
[7] Univ Lyon, Lab Phys, CNRS, UMR 5672, F-69364 Lyon 07, France
[8] Ecole Normale Super Lyon, F-69364 Lyon 07, France
基金
美国国家科学基金会;
关键词
TARGET-SPACE DUALITY; SYMMETRIES; ROTATIONS; SUPERMEMBRANES; SUPERGRAVITY;
D O I
10.1016/j.nuclphysb.2015.10.003
中图分类号
O412 [相对论、场论]; O572.2 [粒子物理学];
学科分类号
摘要
Just as string T-duality originates from transforming field equations into Bianchi identities on the string worldsheet, so it has been suggested that M-theory U-dualities originate from transforming field equations into Bianchi identities on the membrane worldvolume. However, this encounters a problem unless the target space has dimension D = p + 1. We identify the problem to be the nonintegrability of the U-duality transformation assigned to the pull-back map. Just as a double geometry renders manifest the 0(D, D) string T-duality, here we show in the case of the M2-brane in D = 3 that a generalized geometry renders manifest the SL(3) x SL(2) U-duality. In the case of M2-brane in D=4, with and without extra target space coordinates, we show that only the GL(4, R) x R-4 subgroup of the expected SL(5, R) U-duality symmetry is realized. (C) 2015 The Authors. Published by Elsevier B.V.
引用
收藏
页码:1 / 21
页数:21
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