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arxiv: 1704.02136 · v2 · pith:22VZ6XZUnew · submitted 2017-04-07 · 🌌 astro-ph.CO

Constraints on running vacuum model with H(z) and f σ₈

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keywords lambdamodelparameterrunningsigmavacuumacousticalong
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We examine the running vacuum model with $\Lambda (H) = 3 \nu H^2 + \Lambda_0$, where $\nu$ is the model parameter and $\Lambda_0$ is the cosmological constant. From the data of the cosmic microwave background radiation, weak lensing and baryon acoustic oscillation along with the time dependent Hubble parameter $H(z)$ and weighted linear growth $f (z)\sigma_8(z)$ measurements, we find that $\nu=(1.37^{+0.72}_{-0.95})\times 10^{-4}$ with the best fitted $\chi^2$ value slightly smaller than that in the $\Lambda$CDM model.

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