Abstract

We consider a new generalized Chaplygin gas model that includes the original Chaplygin gas model as a special case. In such a model the generalized Chaplygin gas evolves as from dust to quiescence or phantom. We show that the background evolution for the model is equivalent to that for a coupled dark energy model with dark matter. The constraints from the current type Ia supernova data favour a phantom-like Chaplygin gas model.

Highlights

  • Recent observations of type Ia supernovae (SNe Ia) suggest that the expansion of the universe is accelerating and that two-thirds of the total energy density exists in a dark energy component with negative pressure [1]

  • It is easy shown that the background evolution for the variable Chaplygin gas model is equivalent to that for an interaction model between the dark matter and the dark energy with w = −1 + n/6 [20]

  • We have considered a new generalized Chaplygin gas model

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Summary

Introduction

Recent observations of type Ia supernovae (SNe Ia) suggest that the expansion of the universe is accelerating and that two-thirds of the total energy density exists in a dark energy component with negative pressure [1]. One possible approach to constructing a viable model for dark energy is to associate it with a slowly evolving and spatially homogeneous scalar field φ, called “quintessence” [4, 5]. Compared to the original Chaplygin gas, in this generalized model (called as variable Chaplygin gas) the universe tends to be a quiessence-dominated (n > 0) [18] or phantom-dominated one (n < 0) [19] with constant equation of state parameter w = −1 + n/6. It is easy shown that the background evolution for the variable Chaplygin gas model is equivalent to that for an interaction model between the dark matter and the dark energy with w = −1 + n/6 [20].

SN Ia Constraints
Conclusions

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