Observational constraints to Ricci dark energy model by using: SN, BAO, OHD, fgas data sets

被引:52
|
作者
Xu, Lixin [1 ]
Wang, Yuting [1 ]
机构
[1] Dalian Univ Technol, Sch Phys & Optoelect Technol, Inst Theoret Phys, Dalian 116024, Peoples R China
基金
中国国家自然科学基金;
关键词
dark energy experiments; cosmological parameters from CMBR; dark energy theory; HUBBLE-SPACE-TELESCOPE; DIGITAL SKY SURVEY; ANISOTROPY-PROBE OBSERVATIONS; FIELD ELLIPTIC GALAXIES; LUMINOUS RED GALAXIES; COSMOLOGICAL CONSTANT; INTERMEDIATE REDSHIFT; WMAP OBSERVATIONS; ANALYTIC APPROACH; SUPERNOVAE;
D O I
10.1088/1475-7516/2010/06/002
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We perform a global constraint on the Ricci dark energy model with both the flat case and the non-flat case, using the Markov Chain Monte Carlo (MCMC) method and the combined observational data from the cluster X-ray gas mass fraction, Supernovae of type Ia (397), baryon acoustic oscillations, current Cosmic Microwave Background, and the observational Hubble function. In the flat model, we obtain the best fit values of the parameters in 1 sigma, 2 sigma regions: Omega(m0) = 0.2927(-0.0388)(+0.0542), alpha = 0.3823(-0.0418-0.0541)(+0.0331+0.0415), Age/Gyr = 13.48(-0.16-0.21)(+0.13+0.17), H-0 = 69.09(-2.37-3.39)(+2.56+3.09). In the non-flat model, the best fit parameters are found in 1 sigma, 2 sigma regions: Omega(m0) = 0.3003(-0.0371-0.0423)(+0.0367+0.0429), alpha = 0.3845(-0.0474-0.0523)(+0.0386+0.0521), Omega(k) = 0.0240(-0.0130-0.0153)(+0.0109+0.0133), Lambda ge/Cyr = 12.54(-0.37-0.49)(+0.51+0.65), H-0 = 72.89(-3.05-3.72)(+3.31+3.388). Compared to the constraint results in the Lambda CDM model by using the same datasets, it is shown that the current combined datasets prefer the Lambda CDM model to the Ricci dark energy model.
引用
收藏
页数:19
相关论文
共 50 条
  • [31] Observational constraints on tachyonic chameleon dark energy model
    A. Banijamali
    S. Bellucci
    B. Fazlpour
    M. Solbi
    Astrophysics and Space Science, 2018, 363
  • [32] Observational constraints on decaying vacuum dark energy model
    Minglei Tong
    Hyerim Noh
    The European Physical Journal C, 2011, 71
  • [33] Observational constraints on interacting dark matter model without dark energy
    Cao, S.
    Zhu, Z. -H.
    Liang, N.
    ASTRONOMY & ASTROPHYSICS, 2011, 529
  • [34] Observational constraints on the unified dark-energy-dark-matter model
    Wu Pu-Xun
    Yu Hong-Wei
    CHINESE PHYSICS LETTERS, 2007, 24 (03) : 843 - 845
  • [35] Cosmological constraints on dark energy models using DESI BAO 2024
    Zheng, Jie
    Qiang, Da-Chun
    You, Zhi-Qiang
    arXiv,
  • [36] Time-varying dark energy constraints from the latest SN Ia, BAO and SGL
    Zhang, Qing-Jun
    Wu, Yue-Liang
    JOURNAL OF COSMOLOGY AND ASTROPARTICLE PHYSICS, 2010, (08):
  • [37] CMB and BAO constraints for an induced gravity dark energy model with a quartic potential
    Umilta, C.
    Ballardini, M.
    Finelli, F.
    Paoletti, D.
    JOURNAL OF COSMOLOGY AND ASTROPARTICLE PHYSICS, 2015, (08):
  • [38] Constraints from the CMB temperature and other common observational data sets on variable dark energy density models
    Jetzer, Philippe
    Tortora, Crescenzo
    PHYSICAL REVIEW D, 2011, 84 (04):
  • [39] Observational constraints on interacting Tsallis holographic dark energy model
    Sadri, Ehsan
    EUROPEAN PHYSICAL JOURNAL C, 2019, 79 (09):
  • [40] Observational constraints on holographic dark energy model with matter creation
    Ajay Kumar
    C. P. Singh
    Astrophysics and Space Science, 2020, 365