Aspects of supersymmetry breaking driven inflation in orbifold models

Abstract We consider gravitationally induced corrections to inflaton potentials driven by supersymmetry breaking in a five-dimensional supergravity, compactified on a $$ S_1/Z_2 $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:msub> <mml:mi>S</mml:mi> <mml:mn>1</mml:mn> </mml:msub> <mml:mo>/</mml:mo> <mml:msub> <mml:mi>Z</mml:mi> <mml:mn>2</mml:mn> </mml:msub> </mml:mrow> </mml:math> orbifold. The supersymmetry breaking takes place on the hidden brane and is transmitted to the visible brane through finite one loop graphs giving rise to an inflaton potential which includes gravitationally induced terms. These corrections are significant for inflationary cosmology and have the potential to modify the predictions of widely studied supergravity models if the latter are embedded in this framework. To explore these effects we examine two classes of models those inspired by no-scale supergravity models and $$\alpha $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>α</mml:mi> </mml:math> -attractors. Both models are compatible with current cosmological observations but face chalenges in reconciling enhanced values for the scalar power spectrum $$ P_\zeta $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>P</mml:mi> <mml:mi>ζ</mml:mi> </mml:msub> </mml:math> with cosmological data, particularly regarding the tensor to scalar ratio r . In fact $$ P_\zeta \gtrsim 10^{-2}$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:msub> <mml:mi>P</mml:mi> <mml:mi>ζ</mml:mi> </mml:msub> <mml:mo>≳</mml:mo> <mml:msup> <mml:mn>10</mml:mn> <mml:mrow> <mml:mo>-</mml:mo> <mml:mn>2</mml:mn> </mml:mrow> </mml:msup> </mml:mrow> </mml:math> results to $$ r &gt; {\mathcal {O}} (0.1) $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mi>r</mml:mi> <mml:mo>&gt;</mml:mo> <mml:mi>O</mml:mi> <mml:mo>(</mml:mo> <mml:mn>0.1</mml:mn> <mml:mo>)</mml:mo> </mml:mrow> </mml:math> , outside the limits put by current data.

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Journal
The European Physical Journal C
Published
2025-03-27
DOI
https://doi.org/10.1140/epjc/s10052-025-14061-9
Citations
1
Primary Topic
Cosmology and Gravitation Theories
Type
article
Field-Weighted Citation Impact
1.15
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article

Aspects of supersymmetry breaking driven inflation in orbifold models

K. Kaskavelis, G.A. Diamandis, A.B. Lahanas, Georgios A. Pavlopoulos
1 citations
The European Physical Journal C
Cosmology and Gravitation Theories
1.15
article

Aspects of supersymmetry breaking driven inflation in orbifold models

K. Kaskavelis, G.A. Diamandis, A.B. Lahanas, Georgios A. Pavlopoulos
article en
1 citations

Abstract

Abstract We consider gravitationally induced corrections to inflaton potentials driven by supersymmetry breaking in a five-dimensional supergravity, compactified on a $$ S_1/Z_2 $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:msub> <mml:mi>S</mml:mi> <mml:mn>1</mml:mn> </mml:msub> <mml:mo>/</mml:mo> <mml:msub> <mml:mi>Z</mml:mi> <mml:mn>2</mml:mn> </mml:msub> </mml:mrow> </mml:math> orbifold. The supersymmetry breaking takes place on the hidden brane and is transmitted to the visible brane through finite one loop graphs giving rise to an inflaton potential which includes gravitationally induced terms. These corrections are significant for inflationary cosmology and have the potential to modify the predictions of widely studied supergravity models if the latter are embedded in this framework. To explore these effects we examine two classes of models those inspired by no-scale supergravity models and $$\alpha $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>α</mml:mi> </mml:math> -attractors. Both models are compatible with current cosmological observations but face chalenges in reconciling enhanced values for the scalar power spectrum $$ P_\zeta $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>P</mml:mi> <mml:mi>ζ</mml:mi> </mml:msub> </mml:math> with cosmological data, particularly regarding the tensor to scalar ratio r . In fact $$ P_\zeta \gtrsim 10^{-2}$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:msub> <mml:mi>P</mml:mi> <mml:mi>ζ</mml:mi> </mml:msub> <mml:mo>≳</mml:mo> <mml:msup> <mml:mn>10</mml:mn> <mml:mrow> <mml:mo>-</mml:mo> <mml:mn>2</mml:mn> </mml:mrow> </mml:msup> </mml:mrow> </mml:math> results to $$ r &gt; {\mathcal {O}} (0.1) $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mi>r</mml:mi> <mml:mo>&gt;</mml:mo> <mml:mi>O</mml:mi> <mml:mo>(</mml:mo> <mml:mn>0.1</mml:mn> <mml:mo>)</mml:mo> </mml:mrow> </mml:math> , outside the limits put by current data.

The European Physical Journal CVol. 85(3)
National and Kapodistrian University of Athens (GR)
Openalex Percentile: Top 20%
Cosmology and Gravitation Theories
1.15
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