196 research outputs found

    Spectrum of Background X-rays from Moduli Dark Matter

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    We examine the XX-ray spectrum from the decay of the dark-matter moduli with mass ∌O(100)\sim {\cal O}(100)keV, in particular, paying attention to the line spectrum from the moduli trapped in the halo of our galaxy. It is found that with the energy resolution of the current experiments (∌10\sim 10%) the line intensity is about twice stronger than that of the continuum spectrum from the moduli that spread in the whole universe. Therefore, in the future experiments with higher energy resolutions it may be possible to detect such line photons. We also investigate the Îł\gamma-ray spectrum emitted from the decay of the multi-GeV moduli. It is shown that the emitted photons may form MeV-bump in the Îł\gamma-ray spectrum. We also find that if the modulus mass is of the order of 10 GeV, the emitted photons at the peak of the continuum spectrum loses their energy by the scattering and the shape of the spectrum is significantly changed, which makes the constraint weaker than that obtained in the previous works.Comment: 14 pages (RevTeX file) including four postscript figures, reviced version to be published in Physical Review

    Multiple Dp_p-branes as a Dp+2_{p+2}-brane

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    From BFSS matrix theory considerations, it is expected that a single Dp+2_{p+2}-brane action can be obtained from N Dp_p-brane action in large N limit. We examine and confirm this expectation by working out the details of DBI and Chern-Simons terms of Dp+2_{p+2}-brane action from Dp_{p}-brane action. We show that the same relation works for non-BPS, as well as BPS branesComment: 14 page

    Cosmological Moduli Problem in Gauge-mediated Supersymmetry Breaking Theories

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    A generic class of string theories predicts the existence of light moduli fields, and they are expected to have masses mϕm_\phi comparable to the gravitino mass m3/2m_{3/2} which is in a range of 10−210^{-2}keV--1GeV in gauge-mediated supersymmetry breaking theories. Such light fields with weak interactions suppressed by the Planck scale can not avoid some stringent cosmological constraints, that is, they suffer from `cosmological moduli problems'. We show that all the gravitino mass region 10−210^{-2}keV â‰Čm3/2â‰Č\lesssim m_{3/2} \lesssim 1GeV is excluded by the constraints even if we incorporate a late-time mini-inflation (thermal inflation). However, a modification of the original thermal inflation model enables the region 10−210^{-2}keV â‰Čm3/2â‰Č\lesssim m_{3/2} \lesssim 500keV to survive the constraints. It is also stressed that the moduli can be dark matter in our universe for the mass region 10−210^{-2}keV â‰Čmϕâ‰Č\lesssim m_\phi \lesssim 100keV.Comment: A few changes in section IV and

    Cosmological Constraint on the String Dilaton in Gauge-mediated Supersymmetry Breaking Theories

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    The dilaton field in string theories (if exists) is expected to have a mass of the order of the gravitino mass m3/2m_{3/2} which is in a range of 10−210^{-2}keV--1GeV in gauge-mediated supersymmetry breaking models. If it is the case, the cosmic energy density of coherent dilaton oscillation easily exceeds the critical density of the present universe. We show that even if this problem is solved by a late-time entropy production (thermal inflation) a stringent constraint on the energy density of the dilaton oscillation is derived from experimental upperbounds on the cosmic X(Îł\gamma)-ray backgrounds. This excludes an interesting mass region, 500keVâ‰Čm3/2â‰Č1GeV500keV \lesssim m_{3/2} \lesssim 1GeV, in gauge-mediated supersymmetry breaking models.Comment: 13 pages (RevTex file including one figure, use psfig), revised version to be published in Physical Review Letter

    Strong CP and Mu Problems in Theories with Gauge Mediated Supersymmetry Breaking

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    We provide a simple solution to the Ό\mu and strong CP problems in the context of gauge mediated supersymmetry breaking. The generic appearance of R symmetry in dynamical supersymmetry breaking is used to implement Peccei-Quinn symmetry. Acceptable Ό\mu and BB terms as well as the large symmetry breaking scale are induced in the presence of nonrenormalizable interactions. Cosmological consequences of this scheme turn out to yield constraints on the PQ symmetry breaking scale and the number of the messenger/heavy quarks. Complexity in introducing non-R Peccei-Quinn symmetry is contrasted with the case of R symmetry.Comment: 10 pages, Revtex. Significantly modified version to apear in Phys. Rev.

    Adjoint Messengers and Perturbative Unification at the String Scale

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    We consider states in the adjoint representation of the Standard Model gauge group as messengers for mediation of supersymmetry (SUSY) breaking. These new messengers can shift the gauge coupling unification to the string scale at O(5x10^{17} GeV) if their masses are at O(10^{14} GeV). The predicted SUSY mass spectrum at the electroweak scale is significantly different from those in other gauge-mediated or supergravity models, resulting in robust mass relations. The gravitino mass is predicted to be about 1-10 GeV. The heavy messenger sector could provide a superheavy dark matter candidate.Comment: 9 pages, 2 figure

    Cosmological Moduli Problem and Thermal Inflation Models

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    In superstring theories, there exist various dilaton and modulus fields which masses are expected to be of the order of the gravitino mass m3/2m_{3/2}. These fields lead to serious cosmological difficulties, so called ``cosmological moduli problem'', because a large number of moduli particles are produced as the coherent oscillations after the primordial inflation. We make a comprehensive study whether the thermal inflation can solve the cosmological moduli problem in the whole modulus mass region mϕ∌10eV−104GeVm_\phi \sim 10 eV - 10^4 GeV predicted by both hidden sector supersymmetry (SUSY) breaking and gauge-mediated SUSY breaking models. In particular, we take into account the primordial inflation model whose reheating temperature is so low that its reheating process finishes after the thermal inflation ends. We find that the above mass region mϕ(≃m3/2)∌10eV−104GeVm_\phi (\simeq m_{3/2}) \sim 10 eV - 10^4 GeV survives from various cosmological constraints in the presence of the thermal inflation.Comment: 49 pages, 17 figure

    Inflationary models with a flat potential enforced by non-abelian discrete gauge symmetries

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    Non-abelian discrete gauge symmetries can provide the inflaton with a flat potential even when one takes into account gravitational strength effects. The discreteness of the symmetries also provide special field values where inflation can end via a hybrid type mechanism. An interesting feature of this method is that it can naturally lead to extremely flat potentials and so, in principle, to inflation at unusually low energy scales. Two examples of effective field theories with this mechanism are given, one with a hybrid exit and one with a mutated hybrid exit. They include an explicit example in which the single field consistency condition is violated.Comment: 24 pages, uses revtex.sty, submitted to PRD (Nov. 1999) Final version to appear in PRD. Background information on supergravity expande

    Hadronic Axion Model in Gauge-Mediated Supersymmetry Breaking and Cosmology of Saxion

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    Recently we have proposed a simple hadronic axion model within gauge-mediated supersymmetry breaking. In this paper we discuss various cosmological consequences of the model in great detail. A particular attention is paid to a saxion, a scalar partner of an axion, which is produced as a coherent oscillation in the early universe. We show that our model is cosmologically viable, if the reheating temperature of inflation is sufficiently low. We also discuss the late decay of the saxion which gives a preferable power spectrum of the density fluctuation in the standard cold dark matter model when compared with the observation.Comment: 24 pages, 3 figure
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