Advantage of the second-order formalism in double space T-dualization of type II superstring

Abstract In this article we present bosonic T-dualization in double space of the type II superstring theory in the pure spinor formulation. We use the action with constant background fields obtained from the general case under some physically and mathematically justified assumptions. Unlike Nikolić...

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Main Authors: B. Nikolić, B. Sazdović
Format: Article
Language:English
Published: SpringerOpen 2019-10-01
Series:European Physical Journal C: Particles and Fields
Online Access:http://link.springer.com/article/10.1140/epjc/s10052-019-7338-7
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spelling doaj-2b454f3fa2a64dc7b42eedd67b10a8862020-11-25T03:40:00ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522019-10-0179101810.1140/epjc/s10052-019-7338-7Advantage of the second-order formalism in double space T-dualization of type II superstringB. Nikolić0B. Sazdović1Institute of Physics, University of BelgradeInstitute of Physics, University of BelgradeAbstract In this article we present bosonic T-dualization in double space of the type II superstring theory in the pure spinor formulation. We use the action with constant background fields obtained from the general case under some physically and mathematically justified assumptions. Unlike Nikolić and Sazdović (EPJ C 77:197, 2017), where we used the first-order theory, in this article fermionic momenta are integrated out. Full T-dualization in double space is represented as a permutation of the initial $$x^\mu $$ xμ and T-dual coordinates $$y_\mu $$ yμ . Requiring that a T-dual transformation law of the T-dual double coordinate $${}^\star Z^M=(y_\mu ,x^\mu )$$ ⋆ZM=(yμ,xμ) to be of the same form as for initial one $$Z^M=(x^\mu ,y_\mu )$$ ZM=(xμ,yμ) , we obtain the form of the T-dual background fields in terms of the initial ones. The advantage of using the action with integrated fermionic momenta is that it gives all T-dual background fields in terms of the initial ones. In the case of the first-order theory Nikolić and Sazdović (2017) a T-dual R-R field strength was obtained out of the double space formalism under additional assumptions.http://link.springer.com/article/10.1140/epjc/s10052-019-7338-7
collection DOAJ
language English
format Article
sources DOAJ
author B. Nikolić
B. Sazdović
spellingShingle B. Nikolić
B. Sazdović
Advantage of the second-order formalism in double space T-dualization of type II superstring
European Physical Journal C: Particles and Fields
author_facet B. Nikolić
B. Sazdović
author_sort B. Nikolić
title Advantage of the second-order formalism in double space T-dualization of type II superstring
title_short Advantage of the second-order formalism in double space T-dualization of type II superstring
title_full Advantage of the second-order formalism in double space T-dualization of type II superstring
title_fullStr Advantage of the second-order formalism in double space T-dualization of type II superstring
title_full_unstemmed Advantage of the second-order formalism in double space T-dualization of type II superstring
title_sort advantage of the second-order formalism in double space t-dualization of type ii superstring
publisher SpringerOpen
series European Physical Journal C: Particles and Fields
issn 1434-6044
1434-6052
publishDate 2019-10-01
description Abstract In this article we present bosonic T-dualization in double space of the type II superstring theory in the pure spinor formulation. We use the action with constant background fields obtained from the general case under some physically and mathematically justified assumptions. Unlike Nikolić and Sazdović (EPJ C 77:197, 2017), where we used the first-order theory, in this article fermionic momenta are integrated out. Full T-dualization in double space is represented as a permutation of the initial $$x^\mu $$ xμ and T-dual coordinates $$y_\mu $$ yμ . Requiring that a T-dual transformation law of the T-dual double coordinate $${}^\star Z^M=(y_\mu ,x^\mu )$$ ⋆ZM=(yμ,xμ) to be of the same form as for initial one $$Z^M=(x^\mu ,y_\mu )$$ ZM=(xμ,yμ) , we obtain the form of the T-dual background fields in terms of the initial ones. The advantage of using the action with integrated fermionic momenta is that it gives all T-dual background fields in terms of the initial ones. In the case of the first-order theory Nikolić and Sazdović (2017) a T-dual R-R field strength was obtained out of the double space formalism under additional assumptions.
url http://link.springer.com/article/10.1140/epjc/s10052-019-7338-7
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AT bsazdovic advantageofthesecondorderformalismindoublespacetdualizationoftypeiisuperstring
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