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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...

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Detalles Bibliográficos
Autores principales: Burgess, C.P., Grandi, N.E., Quevedo, F., Rabadan, R.
Lenguaje:eng
Publicado: 2003
Materias:
Acceso en línea:https://dx.doi.org/10.1088/1126-6708/2004/01/067
http://cds.cern.ch/record/645879
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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.
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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
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AT grandine dbranechemistry
AT quevedof dbranechemistry
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