50 research outputs found

    Constraints on a new alternative model to dark energy

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    The recent type Ia supernova data suggest that the universe is accelerating now and decelerated in recent past. This may provide the evidence that the standard Friedmann equation needs to be modified. We analyze in detail a new model in the context of modified Friedmann equation using the supernova data published by the High-zz Supernova Search Team and the Supernova Cosmology Project. The new model explains recent acceleration and past deceleration. Furthermore, the new model also gives a decelerated universe in the future.Comment: 12 pages, 5 figures, use ws-ijmpd, minor changes made. In the new version, a detailed derivation of the model is give

    Acceleration from M theory and Fine-tuning

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    The compactification of M theory with time dependent hyperbolic internal space gives an effective scalar field with exponential potential which provides a transient acceleration in Einstein frame in four dimensions. Ordinary matter and radiation are present in addition to the scalar field coming from compactification. We find that we have to fine-tune the initial conditions of the scalar field so that our Universe experiences acceleration now. During the evolution of our Universe, the volume of the internal space increases about 12 times. The time variation of the internal space results in a large time variation of the fine structure constant which violates the observational constraint on the variation of the fine structure constant. The large variation of the fine structure constant is a generic feature of transient acceleration models.Comment: 9 pages, 3 figures, use iopart, v2; references updated, accepted for publication in Class. Quantum Gra

    Observational constraints on dark energy model

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    The recent observations support that our universe is flat and expanding with acceleration. A quintessence model with a general relation between the quintessence potential and the quintessence kinetic energy was proposed to explain the phenomenon. The dark energy potential includes both the hyperbolic and the double exponential potentials. We analyze this model in detail by using the recent supernova and the first year Wilkinson Microwave Anisotropy Probe (WMAP) observations. For a flat universe dominated by a dark energy with constant ω\omega which is a special case of the general model, we find that Ωm0=0.30−0.08+0.06\Omega_{\rm m0}=0.30^{+0.06}_{-0.08} and ωQ≀−0.82\omega_{\rm Q}\le -0.82, and the turnaround redshift zTz_{\rm T} when the universe switched from the deceleration phase to the acceleration phase is zT=0.65z_{\rm T}=0.65. For the general model, we find that Ωm0∌0.3\Omega_{\rm m0}\sim 0.3, ωQ0∌−1.0\omega_{\rm Q0}\sim -1.0, ÎČ∌0.5\beta\sim 0.5 and zT∌0.67z_{\rm T}\sim 0.67. A model independent polynomial parameterization is also considered, the best fit model gives Ωm0=0.40±0.14\Omega_{\rm m0}=0.40\pm 0.14, ωQ0=−1.4\omega_{\rm Q0}=-1.4 and zT=0.37z_{\rm T}=0.37.Comment: 10 pages, 9 figures, update refererences, use ws-ijmpd style, use new supernova data and add model independent analysis. The updated paper also use a new method, fitting the WMAP data, main results remain unchanged. V4: more references added, accepted for publication in Int. J. Mod. Phys.

    Bayesian Analysis of the (Generalized) Chaplygin Gas and Cosmological Constant Models using the 157 gold SNe Ia Data

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    The generalized Chaplygin gas model (GCGM) contains 5 free parameters, here, they are constrained through the type Ia supernovae data, i.e., the ``gold sample'' of 157 supernovae data. Negative and large positive values for α\alpha are taken into account. The analysis is made by employing the Bayesian statistics and the prediction for each parameter is obtained by marginalizing on the remained ones. This procedure leads to the following predictions: α=−0.75−0.24+4.04\alpha = - 0.75^{+4.04}_{-0.24}, H0=65.00−1.75+1.77H_0=65.00^{+1.77}_{-1.75}, Ωk0=−0.77−5.94+1.14\Omega_{k0} = - 0.77^{+1.14}_{-5.94}, Ωm0=0.00−0.00+1.95\Omega_{m0} = 0.00^{+1.95}_{-0.00}, Ωc0=1.36−0.85+5.36\Omega_{c0} = 1.36^{+5.36}_{-0.85}, Aˉ=1.000−0.534+0.000\bar A = 1.000^{+0.000}_{-0.534}. Through the same analysis the specific case of the ordinary Chaplygin gas model (CGM), for which α=1\alpha = 1, is studied. In this case, there are now four free parameters and the predictions for them are: H0=65.01−1.71+1.81H_0 = 65.01^{+1.81}_{-1.71}, Ωk0=−2.73−0.97+1.53\Omega_{k0} = - 2.73^{+1.53}_{-0.97}, Ωm0=0.00−0.00+1.22\Omega_{m0} = 0.00^{+1.22}_{-0.00}, Ωc0=1.34−0.70+0.94\Omega_{c0} = 1.34^{+0.94}_{-0.70}, Aˉ=1.000−0.270+0.000\bar A = 1.000^{+0.000}_{-0.270}. To complete the analysis the Λ\LambdaCDM, with its three free parameters, is considered. For all these models, particular cases are considered where one or two parameters are fixed. The age of the Universe, the deceleration parameter and the moment the Universe begins to accelerate are also evaluated. The quartessence scenario, is favoured. A closed (and in some cases a flat) and accelerating Universe is also preferred. The CGM case α=1\alpha = 1 is far from been ruled out, and it is even preferred in some particular cases. In most of the cases the Λ\LambdaCDM is disfavoured with respect to GCGM and CGM.Comment: 23 pages, LaTeX 2e, 6 tables, 38 EPS figures, uses graphic

    Non-existence of Extended Holographic Dark Energy with Hubble Horizon

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    The extended holographic dark energy model with the Hubble horizon as the infrared cutoff avoids the problem of the circular reasoning of the holographic dark energy model. We show that the infrared cutoff of the extended holographic dark energy model cannot be the Hubble horizon provided that the Brans-Dicke parameter ω\omega satisfies the experimental constraint ω>104\omega> 10^4, and this is proved as a no-go theorem. The no-go theorem also applies to the case in which the dark matter interacts with the dark energy.Comment: 12 pages with revtex, 4 figures, v2: minor corrections to match the version appeared in JCA

    Constraints on alternative models to dark energy

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    The recent observations of type Ia supernovae strongly support that the universe is accelerating now and decelerated in the recent past. This may be the evidence of the breakdown of the standard Friemann equation. We consider a general modified Friedmann equation. Three different models are analyzed in detail. The current supernovae data and the Wilkinson microwave anisotropy probe data are used to constrain these models. A detailed analysis of the transition from the deceleration phase to the acceleration phase is also performed.Comment: 10 pages, 1 figure, revtex

    Testing the viability of the interacting holographic dark energy model by using combined observational constraints

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    Using the data coming from the new 182 Gold type Ia supernova samples, the shift parameter of the Cosmic Microwave Background given by the three-year Wilkinson Microwave Anisotropy Probe observations, and the baryon acoustic oscillation measurement from the Sloan Digital Sky Survey, H(z)H(z) and lookback time measurements, we have performed a statistical joint analysis of the interacting holographic dark energy model. Consistent parameter estimations show us that the interacting holographic dark energy model is a viable candidate to explain the observed acceleration of our universe.Comment: 15 pages, 9 figures, accepted for publication in JCA

    Super-acceleration on the Brane by Energy Flow from the Bulk

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    We consider a brane cosmological model with energy exchange between brane and bulk. Parameterizing the energy exchange term by the scale factor and Hubble parameter, we are able to exactly solve the modified Friedmann equation on the brane. In this model, the equation of state for the effective dark energy has a transition behavior changing from wdeeff>−1w_{de}^{eff}>-1 to wdeeff<−1w_{de}^{eff}<-1, while the equation of state for the dark energy on the brane has w>−1w>-1. Fitting data from type Ia supernova, Sloan Digital Sky Survey and Wilkinson Microwave Anisotropy Probe, our universe is predicted now in the state of super-acceleration with wde0eff=−1.21w_{de0}^{eff}=-1.21.Comment: Revtex, 11 pages including 2 figures,v2: tpos fixed, references added, to appear in JCA

    Constraints on Inflation in Einstein-Brans-Dicke Frame

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    The density perturbation during inflation seeds the large scale structure. We consider both new inflation-type and chaotic inflation-type potentials in the framework of Einstein-Brans-Dicke gravity. The density perturbation gives strong constraints on the parameters in these potentials. For both potentials, the constraints are not much different from those obtained in the original inflationary models by using of Einstein gravity.Comment: 6 pages, Revtex file, typos adde

    PBX3 and MEIS1 Cooperate in Hematopoietic Cells to Drive Acute Myeloid Leukemias Characterized by a Core Transcriptome of the MLL-Rearranged Disease

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    Overexpression of HOXA/MEIS1/PBX3 homeobox genes is the hallmark of mixed lineage leukemia (MLL)-rearranged acute myeloid leukemia (AML). HOXA9 and MEIS1 are considered to be the most critical targets of MLL fusions and their co-expression rapidly induces AML. MEIS1 and PBX3 are not individually able to transform cells and were therefore hypothesized to function as cofactors of HOXA9. However, in this study we demonstrate that co-expression of PBX3 and MEIS1 (PBX3/MEIS1), without ectopic expression of a HOX gene, is sufficient for transformation of normal mouse hematopoietic stem/progenitor cells in vitro. Moreover, PBX3/MEIS1 overexpression also caused AML in vivo, with a leukemic latency similar to that caused by forced expression of MLL-AF9, the most common form of MLL fusions. Furthermore, gene expression profiling of hematopoietic cells demonstrated that PBX3/MEIS1 overexpression, but not HOXA9/MEIS1, HOXA9/PBX3 or HOXA9 overexpression, recapitulated the MLL-fusion-mediated core transcriptome, particularly upregulation of the endogenous Hoxa genes. Disruption of the binding between MEIS1 and PBX3 diminished PBX3/MEIS1-mediated cell transformation and HOX gene upregulation. Collectively, our studies strongly implicate the PBX3/MEIS1 interaction as a driver of cell transformation and leukemogenesis, and suggest that this axis may play a critical role in the regulation of the core transcriptional programs activated in MLL-rearranged and HOX-overexpressing AML. Therefore, targeting the MEIS1/PBX3 interaction may represent a promising therapeutic strategy to treat these AML subtypes
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