N =1 supergravitational heterotic galileons

Abstract Heterotic M -theory consists of a five-dimensional manifold of the form S 1 / Z 2 × M 4. It has been shown that one of the two orbifold planes, the “observable” sector, can have a low energy particle spectrum which is precisely the N = 1 super-symmetric standard model with three right-hande...

Full description

Bibliographic Details
Main Authors: Rehan Deen, Burt Ovrut
Format: Article
Language:English
Published: SpringerOpen 2017-11-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP11(2017)026
id doaj-33db288a9bfc4bbea2ab7dfad6522817
record_format Article
spelling doaj-33db288a9bfc4bbea2ab7dfad65228172020-11-24T23:54:09ZengSpringerOpenJournal of High Energy Physics1029-84792017-11-0120171114010.1007/JHEP11(2017)026N =1 supergravitational heterotic galileonsRehan Deen0Burt Ovrut1Department of Physics and Astronomy, University of PennsylvaniaDepartment of Physics and Astronomy, University of PennsylvaniaAbstract Heterotic M -theory consists of a five-dimensional manifold of the form S 1 / Z 2 × M 4. It has been shown that one of the two orbifold planes, the “observable” sector, can have a low energy particle spectrum which is precisely the N = 1 super-symmetric standard model with three right-handed neutrino chiral supermultiplets. The other orbifold plane constitutes a “hidden” sector which, since its communication with the observable sector is suppressed, will be ignored in this paper. However, the finite fifth-dimension allows for the existence of three-brane solitons which, in order to render the vacuum anomaly free, must appear. That is, heterotic M -theory provides a natural framework for brane-world cosmological scenarios coupled to realistic particle physics. The complete worldvolume action of such three-branes is unknown. Here, treating these solitons as probe branes, we construct their scalar worldvolume Lagrangian as a derivative expansion of the heterotic DBI action. In analogy with similar calculations in the M 5 and AdS 5 context, this leads to the construction of “heterotic Galileons”. However, realistic vacua of heterotic M -theory are necessarily N = 1 supersymmetric in four dimensions. Hence, we proceed to supersymmetrize the three-brane worldvolume action, first in flat superspace and then extend the results to N = 1 supergravity. Such a worldvolume action may lead to interesting cosmology, such as “bouncing” universe models, by allowing for the violation of the Null Energy Condition (NEC).http://link.springer.com/article/10.1007/JHEP11(2017)026p-branesSupergravity ModelsSuperstrings and Heterotic StringsSupersymmetric Effective Theories
collection DOAJ
language English
format Article
sources DOAJ
author Rehan Deen
Burt Ovrut
spellingShingle Rehan Deen
Burt Ovrut
N =1 supergravitational heterotic galileons
Journal of High Energy Physics
p-branes
Supergravity Models
Superstrings and Heterotic Strings
Supersymmetric Effective Theories
author_facet Rehan Deen
Burt Ovrut
author_sort Rehan Deen
title N =1 supergravitational heterotic galileons
title_short N =1 supergravitational heterotic galileons
title_full N =1 supergravitational heterotic galileons
title_fullStr N =1 supergravitational heterotic galileons
title_full_unstemmed N =1 supergravitational heterotic galileons
title_sort n =1 supergravitational heterotic galileons
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2017-11-01
description Abstract Heterotic M -theory consists of a five-dimensional manifold of the form S 1 / Z 2 × M 4. It has been shown that one of the two orbifold planes, the “observable” sector, can have a low energy particle spectrum which is precisely the N = 1 super-symmetric standard model with three right-handed neutrino chiral supermultiplets. The other orbifold plane constitutes a “hidden” sector which, since its communication with the observable sector is suppressed, will be ignored in this paper. However, the finite fifth-dimension allows for the existence of three-brane solitons which, in order to render the vacuum anomaly free, must appear. That is, heterotic M -theory provides a natural framework for brane-world cosmological scenarios coupled to realistic particle physics. The complete worldvolume action of such three-branes is unknown. Here, treating these solitons as probe branes, we construct their scalar worldvolume Lagrangian as a derivative expansion of the heterotic DBI action. In analogy with similar calculations in the M 5 and AdS 5 context, this leads to the construction of “heterotic Galileons”. However, realistic vacua of heterotic M -theory are necessarily N = 1 supersymmetric in four dimensions. Hence, we proceed to supersymmetrize the three-brane worldvolume action, first in flat superspace and then extend the results to N = 1 supergravity. Such a worldvolume action may lead to interesting cosmology, such as “bouncing” universe models, by allowing for the violation of the Null Energy Condition (NEC).
topic p-branes
Supergravity Models
Superstrings and Heterotic Strings
Supersymmetric Effective Theories
url http://link.springer.com/article/10.1007/JHEP11(2017)026
work_keys_str_mv AT rehandeen n1supergravitationalheteroticgalileons
AT burtovrut n1supergravitationalheteroticgalileons
_version_ 1725467015898988544