Spinors fields in co-dimension one braneworlds

Abstract In this work we analyze the zero mode localization and resonances of 1/2−spin fermions in co-dimension one Randall-Sundrum braneworld scenarios. We consider delta-like, domain walls and deformed domain walls membranes. Beyond the influence of the spacetime dimension D we also consider three...

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Main Authors: W.M. Mendes, G. Alencar, R.R. Landim
Format: Article
Language:English
Published: SpringerOpen 2018-02-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP02(2018)018
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spelling doaj-1ef9c3daf11c409ca5e2e33bb39ceeb32020-11-25T00:44:14ZengSpringerOpenJournal of High Energy Physics1029-84792018-02-012018212810.1007/JHEP02(2018)018Spinors fields in co-dimension one braneworldsW.M. Mendes0G. Alencar1R.R. Landim2Departamento de Física, Universidade Federal do CearáDepartamento de Física, Universidade Federal do CearáDepartamento de Física, Universidade Federal do CearáAbstract In this work we analyze the zero mode localization and resonances of 1/2−spin fermions in co-dimension one Randall-Sundrum braneworld scenarios. We consider delta-like, domain walls and deformed domain walls membranes. Beyond the influence of the spacetime dimension D we also consider three types of couplings: (i) the standard Yukawa coupling with the scalar field and parameter η 1, (ii) a Yukawa-dilaton coupling with two parameters η 2 and λ and (iii) a dilaton derivative coupling with parameter h. Together with the deformation parameter s, we end up with five free parameter to be considered. For the zero mode we find that the localization is dependent of D, because the spinorial representation changes when the bulk dimensionality is odd or even and must be treated separately. For case (i) we find that in odd dimensions only one chirality can be localized and for even dimension a massless Dirac spinor is trapped over the brane. In the cases (ii) and (iii) we find that for some values of the parameters, both chiralities can be localized in odd dimensions and for even dimensions we obtain that the massless Dirac spinor is trapped over the brane. We also calculated numerically resonances for cases (ii) and (iii) by using the transfer matrix method. We find that, for deformed defects, the increasing of D induces a shift in the peaks of resonances. For a given λ with domain walls, we find that the resonances can show up by changing the spacetime dimensionality. For example, the same case in D = 5 do not induces resonances but when we consider D = 10 one peak of resonance is found. Therefore the introduction of more dimensions, diversely from the bosonic case, can change drastically the zero mode and resonances in fermion fields.http://link.springer.com/article/10.1007/JHEP02(2018)018Field Theories in Higher DimensionsLarge Extra Dimensions
collection DOAJ
language English
format Article
sources DOAJ
author W.M. Mendes
G. Alencar
R.R. Landim
spellingShingle W.M. Mendes
G. Alencar
R.R. Landim
Spinors fields in co-dimension one braneworlds
Journal of High Energy Physics
Field Theories in Higher Dimensions
Large Extra Dimensions
author_facet W.M. Mendes
G. Alencar
R.R. Landim
author_sort W.M. Mendes
title Spinors fields in co-dimension one braneworlds
title_short Spinors fields in co-dimension one braneworlds
title_full Spinors fields in co-dimension one braneworlds
title_fullStr Spinors fields in co-dimension one braneworlds
title_full_unstemmed Spinors fields in co-dimension one braneworlds
title_sort spinors fields in co-dimension one braneworlds
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2018-02-01
description Abstract In this work we analyze the zero mode localization and resonances of 1/2−spin fermions in co-dimension one Randall-Sundrum braneworld scenarios. We consider delta-like, domain walls and deformed domain walls membranes. Beyond the influence of the spacetime dimension D we also consider three types of couplings: (i) the standard Yukawa coupling with the scalar field and parameter η 1, (ii) a Yukawa-dilaton coupling with two parameters η 2 and λ and (iii) a dilaton derivative coupling with parameter h. Together with the deformation parameter s, we end up with five free parameter to be considered. For the zero mode we find that the localization is dependent of D, because the spinorial representation changes when the bulk dimensionality is odd or even and must be treated separately. For case (i) we find that in odd dimensions only one chirality can be localized and for even dimension a massless Dirac spinor is trapped over the brane. In the cases (ii) and (iii) we find that for some values of the parameters, both chiralities can be localized in odd dimensions and for even dimensions we obtain that the massless Dirac spinor is trapped over the brane. We also calculated numerically resonances for cases (ii) and (iii) by using the transfer matrix method. We find that, for deformed defects, the increasing of D induces a shift in the peaks of resonances. For a given λ with domain walls, we find that the resonances can show up by changing the spacetime dimensionality. For example, the same case in D = 5 do not induces resonances but when we consider D = 10 one peak of resonance is found. Therefore the introduction of more dimensions, diversely from the bosonic case, can change drastically the zero mode and resonances in fermion fields.
topic Field Theories in Higher Dimensions
Large Extra Dimensions
url http://link.springer.com/article/10.1007/JHEP02(2018)018
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AT galencar spinorsfieldsincodimensiononebraneworlds
AT rrlandim spinorsfieldsincodimensiononebraneworlds
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