Current Observational Constraints to Holographic Dark Energy Model with New Infrared cut-off via Markov Chain Monte Carlo Method

preprint2010arXivOpen access

Abstract

In this paper, the holographic dark energy model with new infrared (IR) cut-off for both the flat case and the non-flat case are confronted with the combined constraints of current cosmological observations: type Ia Supernovae, Baryon Acoustic Oscillations, current Cosmic Microwave Background, and the observational hubble data. By utilizing the Markov Chain Monte Carlo (MCMC) method, we obtain the best fit values of the parameters with 1σ,2σ1σ, 2σ errors in the flat model: Ωbh2=0.0233−0.0009−0.0014+0.0009+0.0013Ω_{b}h^2=0.0233^{+0.0009 +0.0013}_{-0.0009 -0.0014}, α=0.8502−0.0875−0.1064+0.0984+0.1299α=0.8502^{+0.0984 +0.1299}_{-0.0875 -0.1064}, β=0.4817−0.0773−0.0955+0.0842+0.1176β=0.4817^{+0.0842 +0.1176}_{-0.0773 -0.0955}, Ωde0=0.7287−0.0294−0.0429+0.0296+0.0432Ω_{de0}=0.7287^{+0.0296 +0.0432}_{-0.0294 -0.0429}, Ωm0=0.2713−0.0296−0.0432+0.0294+0.0429Ω_{m0}=0.2713^{+0.0294 +0.0429}_{-0.0296 -0.0432}, H0=66.35−2.14−3.07+2.38+3.35H_0=66.35^{+2.38 +3.35}_{-2.14 -3.07}. In the non-flat model, the constraint results are found in 1σ,2σ1σ, 2σ regions: Ωbh2=0.0228−0.0010−0.0014+0.0010+0.0014Ω_{b}h^2=0.0228^{+0.0010 +0.0014}_{-0.0010 -0.0014}, Ωk=0.0305−0.0134−0.0176+0.0092+0.0140Ω_k=0.0305^{+0.0092 +0.0140}_{-0.0134 -0.0176}, α=0.8824−0.1163−0.1378+0.2180+0.2213α=0.8824^{+0.2180 +0.2213}_{-0.1163 -0.1378}, β=0.5016−0.0871−0.1102+0.0973+0.1247β=0.5016^{+0.0973 +0.1247}_{-0.0871 -0.1102}, Ωde0=0.6934−0.0304−0.0413+0.0364+0.0495Ω_{de0}=0.6934^{+0.0364 +0.0495}_{-0.0304 -0.0413}, Ωm0=0.2762−0.0320−0.0412+0.0278+0.0402Ω_{m0}=0.2762^{+0.0278 +0.0402}_{-0.0320 -0.0412}, H0=70.20−3.17−4.00+3.03+3.58H_0=70.20^{+3.03 +3.58}_{-3.17 -4.00}. In the best fit holographic dark energy models, the equation of state of dark energy and the deceleration parameter at present are characterized by wde0=−1.1414±0.0608,q0=−0.7476±0.0466w_{de0}=-1.1414\pm0.0608, q_0=-0.7476\pm0.0466 (flat case) and wde0=−1.0653±0.0661,q0=−0.6231±0.0569w_{de0}=-1.0653\pm0.0661, q_0=-0.6231\pm0.0569 (non-flat case). Compared to the ΛCDMΛ\textmd{CDM} model, it is found the current combined datasets do not favor the holographic dark energy model over the ΛCDMΛ\textmd{CDM} model.

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