Statefinder hierarchy exploration of the extended Ricci dark energy

preprint2015arXivOpen access

Abstract

We apply the statefinder hierarchy plus the fractional growth parameter to explore the extended Ricci dark energy (ERDE) model, in which there are two independent coefficients αα and ββ. By adjusting them, we plot evolution trajectories of some typical parameters, including Hubble expansion rate EE, deceleration parameter qq, the third and fourth order hierarchy S3(1)S_3^{(1)} and S4(1)S_4^{(1)} and fractional growth parameter εε, respectively, as well as several combinations of them. For the case of variable αα and constant ββ, in the low-redshift region the evolution trajectories of EE are in high degeneracy and that of qq separate somewhat. However, the ΛΛCDM model is confounded with ERDE in both of these two cases. S3(1)S_3^{(1)} and S4(1)S_4^{(1)}, especially the former, perform much better. They can differentiate well only varieties of cases within ERDE except ΛΛCDM in the low-redshift region. For high-redshift region, combinations {Sn(1),ε}\{S_n^{(1)},ε\} can break the degeneracy. Both of {S3(1),ε}\{S_3^{(1)},ε\} and {S4(1),ε}\{S_4^{(1)},ε\} have the ability to discriminate ERDE with α=1α=1 from ΛΛCDM, of which the degeneracy cannot be broken by all the before-mentioned parameters. For the case of variable ββ and constant αα, S3(1)(z)S_3^{(1)}(z) and S4(1)(z)S_4^{(1)}(z) can only discriminate ERDE from ΛΛCDM. Nothing but pairs {S3(1),ε}\{S_3^{(1)},ε\} and {S4(1),ε}\{S_4^{(1)},ε\} can discriminate not only within ERDE but also ERDE from ΛΛCDM. Finally we find that S3(1)S_3^{(1)} is surprisingly a better choice to discriminate within ERDE itself, and ERDE from ΛΛCDM as well, rather than S4(1)S_4^{(1)}.

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