261 research outputs found

    Quantum Smearing in Hybrid Inflation with Chaotic Potentials

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    We study the impact of one-loop radiative corrections in a non-supersymmetric model of hybrid inflation with chaotic (polynomial-like) potential, V0+λpϕpV_0 + \lambda_p \phi^p. These corrections can arise from the possible couplings of inflaton with other fields which may play active role in the reheating process. The tree-level predictions of these models are shown to lie outside of the Planck's latest bounds on the scalar spectral index nsn_s and the tensor to scalar ratio rr. However, the radiatively corrected version of these models, V0+λpϕp+Aϕ4lnϕ V_0 + \lambda_p \phi^p + A \phi^4 \ln \phi, is fully consistent with the Planck's data. More specifically, fermionic radiative correction (A<0A<0) reduces the tensor to scalar ratio significantly and a red-tilted spectral index ns<1n_s<1, consistent with Planck's data, is obtained even for sub-Planckian field-values.Comment: 14 pages, 25 figures (typos fixed

    Observable Gravity Waves from Supersymmetric Hybrid Inflation II

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    It is shown that a tensor-to-scalar ratio close to r = 0.03, which can be observed by Planck, is realized in supersymmetric hybrid inflation models with TeV-scale soft supersymmetry breaking terms. This extends our previous analysis, which also found r <~ 0.03 but employed intermediate scale soft terms. Other cosmological observables such as the scalar spectral index are in good agreement with the WMAP data.Comment: 4 pages, 4 figure

    Amelioration of Little Hierarchy Problem in SU(4)_c x SU(2)_L x SU(2)_R

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    The little hierarchy problem encountered in the constrained minimal supersymmetric model (CMSSM) can be ameliorated in supersymmetric models based on the gauge symmetry G_{422} \equiv SU(4)_c x SU(2)_L x SU(2)_R. The standard assumption in CMSSM (and in SU(5) and SO(10)) of universal gaugino masses can be relaxed in G_{422}, and this leads to a significant improvement in the degree of fine tuning required to implement radiative electroweak breaking in the presence of a characteristic supersymmetry breaking scale of around a TeV. Examples of Higgs and sparticle mass spectra realized with 10% fine tuning are presented.Comment: 14 pages, 5 figures, 2 table

    Higgs Boson Mass, Sparticle Spectrum and Little Hierarchy Problem in Extended MSSM

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    We investigate the impact of TeV-scale matter belonging to complete vectorlike multiplets of unified groups on the lightest Higgs boson in the MSSM. We find that consistent with perturbative unification and electroweak precision data the mass m_h can be as large as 160 GeV. These extended MSSM models can also render the little hierarchy problem less severe, but only for lower values of m_h < 125 GeV. We present estimates for the sparticle mass spectrum in these models.Comment: 27 pages, 14 figure

    Red Spectral Tilt and Observable Gravity Waves in Shifted Hybrid Inflation

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    We consider supersymmetric shifted hybrid inflation models with a red tilted scalar spectral index n_s in agreement with the WMAP 7-yr central value. If non-minimal supergravity corrections are included, these models can also support a tensor-to-scalar ratio as large as r = 0.02, which may be observable by the Planck Satellite. In contrast to the standard supersymmetric hybrid inflation scenario, topological defects produced via gauge symmetry breaking are inflated away in the shifted version of the theory.Comment: 22 pages, 4 figures, and 1 tabl

    Higgs Inflation, Quantum Smearing and the Tensor to Scalar Ratio

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    In cosmic inflation driven by a scalar gauge singlet field with a tree level Higgs potential, the scalar to tensor ratio r is estimated to be larger than 0.036, provided the scalar spectral index n_s >= 0.96. We discuss quantum smearing of these predictions arising from the inflaton couplings to other particles such as GUT scalars, and show that these corrections can significantly decrease r. However, for n_s >= 0.96, we obtain r >= 0.02 which can be tested by the Planck satellite.Comment: 10 pages, 3 figures and 3 table
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