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D-Brane Chemistry
We study several different kinds of bound states built from D-branes and orientifolds. These states are to atoms what branonium - the bound state of a brane and its anti-brane - is to positronium, inasmuch as they typically involve a light brane bound to a much heavier object with conserved charges...
Autores principales: | , , , |
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Lenguaje: | eng |
Publicado: |
2003
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1088/1126-6708/2004/01/067 http://cds.cern.ch/record/645879 |
_version_ | 1780900850441388032 |
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author | Burgess, C.P. Grandi, N.E. Quevedo, F. Rabadan, R. |
author_facet | Burgess, C.P. Grandi, N.E. Quevedo, F. Rabadan, R. |
author_sort | Burgess, C.P. |
collection | CERN |
description | We study several different kinds of bound states built from D-branes and orientifolds. These states are to atoms what branonium - the bound state of a brane and its anti-brane - is to positronium, inasmuch as they typically involve a light brane bound to a much heavier object with conserved charges which forbid the system's decay. We find the fully relativistic motion of a probe Dp'-brane in the presence of source Dp-branes is integrable by quadratures. Keplerian conic sections are obtained for special choices for p and p' and the systems are shown to be equivalent to nonrelativistic systems. Their quantum behaviour is also equivalent to the corresponding non-relativistic limit. In particular the p=6, p'=0 case is equivalent to a non-relativistic dyon in a magnetic monopole background, with the trajectories in the surface of a cone. We also show that the motion of the probe branes about D6-branes in IIA theory is equivalent to the motion of the corresponding probes in the uplift to M-theory in 11 dimensions, for which there are no D6-branes but their fields are replaced by a particular Taub-NUT geometry. We further discuss the interactions of D-branes and orientifold planes having the same dimension. this system behaves at large distances as a brane-brane system but at shorter distances it does not have the tachyon instability. |
id | cern-645879 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2003 |
record_format | invenio |
spelling | cern-6458792023-03-14T20:04:40Zdoi:10.1088/1126-6708/2004/01/067http://cds.cern.ch/record/645879engBurgess, C.P.Grandi, N.E.Quevedo, F.Rabadan, R.D-Brane ChemistryParticle Physics - TheoryWe study several different kinds of bound states built from D-branes and orientifolds. These states are to atoms what branonium - the bound state of a brane and its anti-brane - is to positronium, inasmuch as they typically involve a light brane bound to a much heavier object with conserved charges which forbid the system's decay. We find the fully relativistic motion of a probe Dp'-brane in the presence of source Dp-branes is integrable by quadratures. Keplerian conic sections are obtained for special choices for p and p' and the systems are shown to be equivalent to nonrelativistic systems. Their quantum behaviour is also equivalent to the corresponding non-relativistic limit. In particular the p=6, p'=0 case is equivalent to a non-relativistic dyon in a magnetic monopole background, with the trajectories in the surface of a cone. We also show that the motion of the probe branes about D6-branes in IIA theory is equivalent to the motion of the corresponding probes in the uplift to M-theory in 11 dimensions, for which there are no D6-branes but their fields are replaced by a particular Taub-NUT geometry. We further discuss the interactions of D-branes and orientifold planes having the same dimension. this system behaves at large distances as a brane-brane system but at shorter distances it does not have the tachyon instability.We study several different kinds of bound states built from D-branes and orientifolds. These states are to atoms what branonium - the bound state of a brane and its anti-brane - is to positronium, inasmuch as they typically involve a light brane bound to a much heavier object with conserved charges which forbid the system's decay. We find the fully relativistic motion of a probe Dp'-brane in the presence of source Dp-branes is integrable by quadratures. Keplerian conic sections are obtained for special choices for p and p' and the systems are shown to be equivalent to nonrelativistic systems. Their quantum behaviour is also equivalent to the corresponding non-relativistic limit. In particular the p=6, p'=0 case is equivalent to a non-relativistic dyon in a magnetic monopole background, with the trajectories in the surface of a cone. We also show that the motion of the probe branes about D6-branes in IIA theory is equivalent to the motion of the corresponding probes in the uplift to M-theory in 11 dimensions, for which there are no D6-branes but their fields are replaced by a particular Taub-NUT geometry. We further discuss the interactions of D-branes and orientifold planes having the same dimension. this system behaves at large distances as a brane-brane system but at shorter distances it does not have the tachyon instability.hep-th/0310010MCGILL-03-18DAMTP-2003-89CERN-TH-2003-193CERN-TH-2003-193DAMTP-2003-89MCGILL-2003-18oai:cds.cern.ch:6458792003-10-01 |
spellingShingle | Particle Physics - Theory Burgess, C.P. Grandi, N.E. Quevedo, F. Rabadan, R. D-Brane Chemistry |
title | D-Brane Chemistry |
title_full | D-Brane Chemistry |
title_fullStr | D-Brane Chemistry |
title_full_unstemmed | D-Brane Chemistry |
title_short | D-Brane Chemistry |
title_sort | d-brane chemistry |
topic | Particle Physics - Theory |
url | https://dx.doi.org/10.1088/1126-6708/2004/01/067 http://cds.cern.ch/record/645879 |
work_keys_str_mv | AT burgesscp dbranechemistry AT grandine dbranechemistry AT quevedof dbranechemistry AT rabadanr dbranechemistry |