de Sitter swampland conjecture in string field inflation

Abstract In this paper, we study a particular type of inflation by using non-local Friedman equations that are derived from the zero levels of string field theory and express a tachyonic action. Then, we challenge it by further refining de Sitter (dS) swampland conjecture (FRdSSC) monitoring. Theref...

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Main Authors: J. Sadeghi, B. Pourhassan, S. Noori Gashti, İ. Sakallı, M. R. Alipour
Format: Article
Language:English
Published: SpringerOpen 2023-07-01
Series:European Physical Journal C: Particles and Fields
Online Access:https://doi.org/10.1140/epjc/s10052-023-11822-2
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author J. Sadeghi
B. Pourhassan
S. Noori Gashti
İ. Sakallı
M. R. Alipour
author_facet J. Sadeghi
B. Pourhassan
S. Noori Gashti
İ. Sakallı
M. R. Alipour
author_sort J. Sadeghi
collection DOAJ
description Abstract In this paper, we study a particular type of inflation by using non-local Friedman equations that are derived from the zero levels of string field theory and express a tachyonic action. Then, we challenge it by further refining de Sitter (dS) swampland conjecture (FRdSSC) monitoring. Therefore, we investigate some quantities, such as potential and Hubble parameters. We also consider slow-roll parameters to examine quantities such as the scalar spectrum index and the tensor-to-scalar ratio. Using straightforward calculations, we investigate this model from the swampland conjecture perspective in terms of the cosmological parameters, i.e., ( $$n_s$$ n s ), (r), and observable data such as Planck 2018, by constructing some structures such as $$(c_{1,2}-n_s)$$ ( c 1 , 2 - n s ) and $$(c_{1,2}-r_s)$$ ( c 1 , 2 - r s ) . Then, we make a new restriction for this conjecture as $$c_1^2c_2^2$$ c 1 2 c 2 2 and get a limit for this model in the range $$c<0.0942$$ c < 0.0942 . We find this inflationary model is strongly in tension with the dS swampland conjecture (dSSC), i.e., $$c_1=c_2 \ne {\mathcal {O}}(1)$$ c 1 = c 2 ≠ O ( 1 ) . So, we shall challenge it with the FRdSSC, which has some free parameters, viz., $$a,b>0$$ a , b > 0 , $$a+b=1$$ a + b = 1 , and $$q>2$$ q > 2 . By setting these parameters, we examine the compatibility of the mentioned conjecture with this inflationary model. Finally, we infer from this string field inflation (SFI) model that it satisfies the FRdSSC with the constraint of its free parameters a, b, and q.
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spelling doaj.art-0fdb78b8821f497eb0ab9a614640cd762023-09-10T11:24:24ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60522023-07-0183711110.1140/epjc/s10052-023-11822-2de Sitter swampland conjecture in string field inflationJ. Sadeghi0B. Pourhassan1S. Noori Gashti2İ. Sakallı3M. R. Alipour4Department of Physics, Faculty of Basic Sciences, University of MazandaranSchool of Physics, Damghan UniversitySchool of Physics, Damghan UniversityPhysics Department, Eastern Mediterranean UniversityDepartment of Physics, Faculty of Basic Sciences, University of MazandaranAbstract In this paper, we study a particular type of inflation by using non-local Friedman equations that are derived from the zero levels of string field theory and express a tachyonic action. Then, we challenge it by further refining de Sitter (dS) swampland conjecture (FRdSSC) monitoring. Therefore, we investigate some quantities, such as potential and Hubble parameters. We also consider slow-roll parameters to examine quantities such as the scalar spectrum index and the tensor-to-scalar ratio. Using straightforward calculations, we investigate this model from the swampland conjecture perspective in terms of the cosmological parameters, i.e., ( $$n_s$$ n s ), (r), and observable data such as Planck 2018, by constructing some structures such as $$(c_{1,2}-n_s)$$ ( c 1 , 2 - n s ) and $$(c_{1,2}-r_s)$$ ( c 1 , 2 - r s ) . Then, we make a new restriction for this conjecture as $$c_1^2c_2^2$$ c 1 2 c 2 2 and get a limit for this model in the range $$c<0.0942$$ c < 0.0942 . We find this inflationary model is strongly in tension with the dS swampland conjecture (dSSC), i.e., $$c_1=c_2 \ne {\mathcal {O}}(1)$$ c 1 = c 2 ≠ O ( 1 ) . So, we shall challenge it with the FRdSSC, which has some free parameters, viz., $$a,b>0$$ a , b > 0 , $$a+b=1$$ a + b = 1 , and $$q>2$$ q > 2 . By setting these parameters, we examine the compatibility of the mentioned conjecture with this inflationary model. Finally, we infer from this string field inflation (SFI) model that it satisfies the FRdSSC with the constraint of its free parameters a, b, and q.https://doi.org/10.1140/epjc/s10052-023-11822-2
spellingShingle J. Sadeghi
B. Pourhassan
S. Noori Gashti
İ. Sakallı
M. R. Alipour
de Sitter swampland conjecture in string field inflation
European Physical Journal C: Particles and Fields
title de Sitter swampland conjecture in string field inflation
title_full de Sitter swampland conjecture in string field inflation
title_fullStr de Sitter swampland conjecture in string field inflation
title_full_unstemmed de Sitter swampland conjecture in string field inflation
title_short de Sitter swampland conjecture in string field inflation
title_sort de sitter swampland conjecture in string field inflation
url https://doi.org/10.1140/epjc/s10052-023-11822-2
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AT bpourhassan desitterswamplandconjectureinstringfieldinflation
AT snoorigashti desitterswamplandconjectureinstringfieldinflation
AT isakallı desitterswamplandconjectureinstringfieldinflation
AT mralipour desitterswamplandconjectureinstringfieldinflation