[Théorie des champs des supertubes]
Considérant des M2-branes s'intersectant en théorie M, le supertube pour la théorie de type IIA est déduite par une compactification sur et un boost à la vitesse de la lumière selon la 11ème dimension. Une procédure similaire est appliquée aux instantons de Donaldson–Uhlenbeck–Yau sur , qui sont vus comme des intersections de membranes de la théorie supersymétrique de Yang–Mills (SYM) en , donnant (pour un boost fini) un ensemble nouveau d'équations BPS pour la théorie de SYM-Higgs en , et (pour un boost infini) une généralisation des équations d'instantons dyoniques de la théorie SYM-Higgs en , solutions qui sont interprétées commes des supertubes de Yang–Mills et réalisées comme des configurations de la théorie des cordes de type IIB.
Starting with intersecting M2-branes in M-theory, the IIA supertube can be found by compactification followed by a boost to the speed of light in the 11th dimension. A similar procedure applied to Donaldson–Uhlenbeck–Yau instantons on , viewed as intersecting membranes of supersymmetric Yang–Mills (SYM) theory, yields (for finite boost) a new set of BPS equations for SYM-Higgs theory, and (for infinite boost) a generalization of the dyonic instanton equations of SYM-Higgs theory, solutions of which are interpreted as Yang–Mills supertubes and realized as configurations of IIB string theory.
Mot clés : Théorie des cordes, Supertube, Théorie de Yang–Mills
@article{CRPHYS_2005__6_2_271_0,
author = {Paul K. Townsend},
title = {Field theory supertubes},
journal = {Comptes Rendus. Physique},
pages = {271--277},
publisher = {Elsevier},
volume = {6},
number = {2},
year = {2005},
doi = {10.1016/j.crhy.2004.12.012},
language = {en},
}
Paul K. Townsend. Field theory supertubes. Comptes Rendus. Physique, Volume 6 (2005) no. 2, pp. 271-277. doi : 10.1016/j.crhy.2004.12.012. https://comptes-rendus.academie-sciences.fr/physique/articles/10.1016/j.crhy.2004.12.012/
[1] D-brane solitons in supersymmetric sigma-models, Phys. Rev. D, Volume 63 (2001), p. 085002 | arXiv
[2] Supertubes, Phys. Rev. Lett., Volume 87 (2001), p. 011602 | arXiv
[3] Supertubes and supercurves from M-ribbons, Phys. Lett. B, Volume 539 (2002), p. 153 | arXiv
[4] Properties of the eleven-dimensional super membrane theory, Ann. Phys., Volume 189 (1987), p. 75
[5] Supergravity supertubes, JHEP, Volume 0107 (2001), p. 011 | arXiv
[6] Sigma-model soliton intersections from exceptional calibrations, JHEP, Volume 0204 (2002), p. 039 | arXiv
[7] Nonlinear sigma models and their Q lump solutions, Phys. Lett. B, Volume 366 (1991), p. 283
[8] More on Q kinks: A ()-dimensional analog of dyons, Phys. Lett. B, Volume 295 (1992), p. 225
[9] Dyonic instantons in five-dimensional gauge theories, Phys. Lett. B, Volume 462 (1999), p. 89 | arXiv
[10] BPS equations in six and eight dimensions, Phys. Rev. D, Volume 66 (2002), p. 025021 | arXiv
[11] Noncommutative instantons in higher dimensions, vortices and topological K-cycles, JHEP, Volume 419 (1998), p. 167 | arXiv
[12] Aspects of supertubes, JHEP, Volume 0205 (2002), p. 017 | arXiv
[13] Supertubes connecting D4 branes, Phys. Lett. B, Volume 544 (2002), p. 329 | arXiv
[14] The heterotic dyonic instanton, JHEP, Volume 0105 (2001), p. 046 | arXiv
[15] Dyonic instanton as supertube between D4 branes, JHEP, Volume 0309 (2003), p. 035 | arXiv
[16] Geometry of the nonabelian DBI dyonic instanton, Phys. Lett. B, Volume 493 (2000), p. 411 | arXiv
[17] Supersymmetric D2 anti-D2 strings, Phys. Lett. B, Volume 626 (2002), p. 165 | arXiv
[18] Tachyons, supertubes and brane/anti-brane systems, JHEP, Volume 0203 (2002), p. 016 | arXiv
[19] Fuzzy BIon, Phys. Rev. D, Volume 509 (2001), p. 168 | arXiv
Cité par Sources :
Commentaires - Politique