Numerical Polynomial Homotopy Continuation Method and String Vacua

Finding vacua for the four-dimensional effective theories for supergravity which descend from flux compactifications and analyzing them according to their stability is one of the central problems in string phenomenology. Except for some simple toy models, it is, however, difficult to find all the va...

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Main Author: Dhagash Mehta
Format: Article
Language:English
Published: Hindawi Limited 2011-01-01
Series:Advances in High Energy Physics
Online Access:http://dx.doi.org/10.1155/2011/263937
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spelling doaj-ad4b3503aeba4d87a3658c3588597bd32020-11-24T22:34:30ZengHindawi LimitedAdvances in High Energy Physics1687-73571687-73652011-01-01201110.1155/2011/263937263937Numerical Polynomial Homotopy Continuation Method and String VacuaDhagash Mehta0Physics Department, Syracuse University, Syracuse, NY 13244, USAFinding vacua for the four-dimensional effective theories for supergravity which descend from flux compactifications and analyzing them according to their stability is one of the central problems in string phenomenology. Except for some simple toy models, it is, however, difficult to find all the vacua analytically. Recently developed algorithmic methods based on symbolic computer algebra can be of great help in the more realistic models. However, they suffer from serious algorithmic complexities and are limited to small system sizes. In this paper, we review a numerical method called the numerical polynomial homotopy continuation (NPHC) method, first used in the areas of lattice field theories, which by construction finds all of the vacua of a given potential that is known to have only isolated solutions. The NPHC method is known to suffer from no major algorithmic complexities and is embarrassingly parallelizable, and hence its applicability goes way beyond the existing symbolic methods. We first solve a simple toy model as a warm-up example to demonstrate the NPHC method at work. We then show that all the vacua of a more complicated model of a compactified M theory model, which has an SU(3) structure, can be obtained by using a desktop machine in just about an hour, a feat which was reported to be prohibitively difficult by the existing symbolic methods. Finally, we compare the various technicalities between the two methods.http://dx.doi.org/10.1155/2011/263937
collection DOAJ
language English
format Article
sources DOAJ
author Dhagash Mehta
spellingShingle Dhagash Mehta
Numerical Polynomial Homotopy Continuation Method and String Vacua
Advances in High Energy Physics
author_facet Dhagash Mehta
author_sort Dhagash Mehta
title Numerical Polynomial Homotopy Continuation Method and String Vacua
title_short Numerical Polynomial Homotopy Continuation Method and String Vacua
title_full Numerical Polynomial Homotopy Continuation Method and String Vacua
title_fullStr Numerical Polynomial Homotopy Continuation Method and String Vacua
title_full_unstemmed Numerical Polynomial Homotopy Continuation Method and String Vacua
title_sort numerical polynomial homotopy continuation method and string vacua
publisher Hindawi Limited
series Advances in High Energy Physics
issn 1687-7357
1687-7365
publishDate 2011-01-01
description Finding vacua for the four-dimensional effective theories for supergravity which descend from flux compactifications and analyzing them according to their stability is one of the central problems in string phenomenology. Except for some simple toy models, it is, however, difficult to find all the vacua analytically. Recently developed algorithmic methods based on symbolic computer algebra can be of great help in the more realistic models. However, they suffer from serious algorithmic complexities and are limited to small system sizes. In this paper, we review a numerical method called the numerical polynomial homotopy continuation (NPHC) method, first used in the areas of lattice field theories, which by construction finds all of the vacua of a given potential that is known to have only isolated solutions. The NPHC method is known to suffer from no major algorithmic complexities and is embarrassingly parallelizable, and hence its applicability goes way beyond the existing symbolic methods. We first solve a simple toy model as a warm-up example to demonstrate the NPHC method at work. We then show that all the vacua of a more complicated model of a compactified M theory model, which has an SU(3) structure, can be obtained by using a desktop machine in just about an hour, a feat which was reported to be prohibitively difficult by the existing symbolic methods. Finally, we compare the various technicalities between the two methods.
url http://dx.doi.org/10.1155/2011/263937
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