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D-Branes at Singularities: A Bottom-Up Approach to the String Embedding of the Standard Model
We propose a bottom-up approach to the building of particle physics models from string theory. Our building blocks are Type II D-branes which we combine appropriately to reproduce desirable features of a particle theory model: 1) Chirality ; 2) Standard Model group ; 3) N=1 or N=0 supersymmetry ; 4)...
Autores principales: | , , , |
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Lenguaje: | eng |
Publicado: |
2000
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1088/1126-6708/2000/08/002 http://cds.cern.ch/record/436962 |
_version_ | 1780895462177374208 |
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author | Aldazabal, G. Ibanez, Luis E. Quevedo, F. Uranga, A.M. |
author_facet | Aldazabal, G. Ibanez, Luis E. Quevedo, F. Uranga, A.M. |
author_sort | Aldazabal, G. |
collection | CERN |
description | We propose a bottom-up approach to the building of particle physics models from string theory. Our building blocks are Type II D-branes which we combine appropriately to reproduce desirable features of a particle theory model: 1) Chirality ; 2) Standard Model group ; 3) N=1 or N=0 supersymmetry ; 4) Three quark-lepton generations. We start such a program by studying configurations of D=10, Type IIB D3-branes located at singularities. We study in detail the case of Z_N, N=1,0 supersymmetric orbifold singularities leading to the SM group or some left-right symmetricextension. In general, tadpole cancellation conditions require the presence of additional branes, e.g. D7-branes. For the N=1 supersymmetric case the unique twist leading to three quark-lepton generations is Z_3, predicting $\sin^2\theta_W=3/14=0.21$. The models obtained are the simplest semirealistic string models ever built. In the non-supersymmetric case there is a three-generation model for each Z_N, N>4, but the Weinberg angle is in general too small. One can obtain a large class of D=4 compact models by considering the above structure embedded into a Calabi Yau compactification. We explicitly construct examples of such compact models using Z_3 toroidal orbifolds and orientifolds, and discuss their properties. In these examples, global cancellation of RR charge may be achieved by adding anti-branes stuck at the fixed points, leading to models with hidden sector gravity-induced supersymmetry breaking. More general frameworks, like F-theory compactifications, allow completely $\NN=1$ supersymmetric embeddings of our local structures, as we show in an explicit example. |
id | cern-436962 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2000 |
record_format | invenio |
spelling | cern-4369622019-09-30T06:29:59Zdoi:10.1088/1126-6708/2000/08/002http://cds.cern.ch/record/436962engAldazabal, G.Ibanez, Luis E.Quevedo, F.Uranga, A.M.D-Branes at Singularities: A Bottom-Up Approach to the String Embedding of the Standard ModelParticle Physics - TheoryWe propose a bottom-up approach to the building of particle physics models from string theory. Our building blocks are Type II D-branes which we combine appropriately to reproduce desirable features of a particle theory model: 1) Chirality ; 2) Standard Model group ; 3) N=1 or N=0 supersymmetry ; 4) Three quark-lepton generations. We start such a program by studying configurations of D=10, Type IIB D3-branes located at singularities. We study in detail the case of Z_N, N=1,0 supersymmetric orbifold singularities leading to the SM group or some left-right symmetricextension. In general, tadpole cancellation conditions require the presence of additional branes, e.g. D7-branes. For the N=1 supersymmetric case the unique twist leading to three quark-lepton generations is Z_3, predicting $\sin^2\theta_W=3/14=0.21$. The models obtained are the simplest semirealistic string models ever built. In the non-supersymmetric case there is a three-generation model for each Z_N, N>4, but the Weinberg angle is in general too small. One can obtain a large class of D=4 compact models by considering the above structure embedded into a Calabi Yau compactification. We explicitly construct examples of such compact models using Z_3 toroidal orbifolds and orientifolds, and discuss their properties. In these examples, global cancellation of RR charge may be achieved by adding anti-branes stuck at the fixed points, leading to models with hidden sector gravity-induced supersymmetry breaking. More general frameworks, like F-theory compactifications, allow completely $\NN=1$ supersymmetric embeddings of our local structures, as we show in an explicit example.We propose a bottom-up approach to the building of particle physics models from string theory. Our building blocks are Type II D-branes which we combine appropriately to reproduce desirable features of a particle theory model: 1) Chirality ; 2) Standard Model group ; 3) N=1 or N=0 supersymmetry ; 4) Three quark-lepton generations. We start such a program by studying configurations of D=10, Type IIB D3-branes located at singularities. We study in detail the case of Z_N, N=1,0 orbifold singularities leading to the SM group or some left-right symmetricextension. In general, tadpole cancellation conditions require the presence of additional branes, e.g. D7-branes. For the N=1 supersymmetric case the unique twist leading to three quark-lepton generations is Z_3, predicting $\sin^2\theta_W=3/14=0.21$. The models obtained are the simplest semirealistic string models ever built. In the non-supersymmetric case there is a three-generation model for each Z_N, N>4, but the Weinberg angle is in general too small. One can obtain a large class of D=4 compact models by considering the above structure embedded into a Calabi Yau compactification. We explicitly construct examples of such compact models using Z_3 toroidal orbifolds and orientifolds, and discuss their properties. In these examples, global cancellation of RR charge may be achieved by adding anti-branes stuck at the fixed points, leading to models with hidden sector gravity-induced supersymmetry breaking. More general frameworks, like F-theory compactifications, allow completely $\NN=1$ supersymmetric embeddings of our local structures, as we show in an explicit example.hep-th/0005067FTUAM-00-10IFT-UAM-CSIC-00-18DAMTP-2000-42CAB-IB-2405300CERN-TH-2000-127CAB-IB-524CERN-TH-2000-127DAMTP-2000-42FTUAM-2000-10IFT-UAM-CSIC-2000-18oai:cds.cern.ch:4369622000-05-08 |
spellingShingle | Particle Physics - Theory Aldazabal, G. Ibanez, Luis E. Quevedo, F. Uranga, A.M. D-Branes at Singularities: A Bottom-Up Approach to the String Embedding of the Standard Model |
title | D-Branes at Singularities: A Bottom-Up Approach to the String Embedding of the Standard Model |
title_full | D-Branes at Singularities: A Bottom-Up Approach to the String Embedding of the Standard Model |
title_fullStr | D-Branes at Singularities: A Bottom-Up Approach to the String Embedding of the Standard Model |
title_full_unstemmed | D-Branes at Singularities: A Bottom-Up Approach to the String Embedding of the Standard Model |
title_short | D-Branes at Singularities: A Bottom-Up Approach to the String Embedding of the Standard Model |
title_sort | d-branes at singularities: a bottom-up approach to the string embedding of the standard model |
topic | Particle Physics - Theory |
url | https://dx.doi.org/10.1088/1126-6708/2000/08/002 http://cds.cern.ch/record/436962 |
work_keys_str_mv | AT aldazabalg dbranesatsingularitiesabottomupapproachtothestringembeddingofthestandardmodel AT ibanezluise dbranesatsingularitiesabottomupapproachtothestringembeddingofthestandardmodel AT quevedof dbranesatsingularitiesabottomupapproachtothestringembeddingofthestandardmodel AT urangaam dbranesatsingularitiesabottomupapproachtothestringembeddingofthestandardmodel |