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arXiv 0904.4496gr-qc
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函数q(z)作为宇宙学参数的一致性检验

The function q(z) as a consistency check for cosmological parameters

M. L. Bedran

摘要:

在弗里德曼宇宙学中,膨胀q的减速起着基本的作用。在不假设空间平坦性的情况下,我们推导了在$Λ$ CDM模型和修正的Chaubergin气体(MCG)模型下,减速随红移$q(z)$的变化.得到了从减速膨胀到加速膨胀的跃迁红移$z_t$与宇宙学参数之间的关系式,其中没有曲率参数。当然,$z_t$的数值取决于$Ω_k$,因为$Ω_L + Ω_M + Ω_k = 1$。精确函数$q(z)$允许计算平坦$Λ$ CDM模型在$z \approx 0.1$处的感染点。这个拐点在Daly和Djorgovski,Ap.J.612,652(2004)的工作的图5中可见,其中减速直接从观测数据绘制。我们还考虑了曲率的小贡献的可能性,即$Ω_k = - 0.1 Ω_L $,并计算出跃迁红移为$z_t = 0.56$,它落在Riess等人获得的区间$0.46 \pm 0.13$内,Ap.J.607,665(2004)。MCG模型计算的跃迁红移比$z_t \approx 0.2$低得多,但观测数据并不排除纯的Chaubergin气体。

英文摘要:

In the Friedmann cosmology the deceleration of the expansion q plays a fundamental role. We derive the deceleration as a function of redshift $q(z)$ in two scenarios: $Λ$ CDM model and modified Chaplygin gas (MCG) model, without assuming spatial flatness. The expression relating the transition redshift from decelerated to accelerated expansion $z_t$ to the cosmological parameters is obtained; it is seen that the curvature parameter does not appear in this expression. Of course the numerical value of $z_t$ depends on $Ω_k$, since $Ω_L + Ω_M + Ω_k = 1$. The exact function $q(z)$ allows the calculation of an infection point at $z \approx 0.1$ for the flat $Λ$ CDM model. This inflection point is visible in Fig.5 of the work of Daly and Djorgovski, Ap.J. 612,652 (2004), where the deceleration was plotted directly from observational data. We also consider the possibility of a small contribution of the curvature, namely, $Ω_k = - 0.1 Ω_L $, and calculate the transition redshift to be $z_t = 0.56$, which falls inside the interval $0.46 \pm 0.13$ obtained by Riess et al., Ap.J. 607, 665 (2004). The calculated transition redshift for the MCG model is considerably lower $z_t \approx 0.2$, but the observational data do not exclude a pure Chaplygin gas.

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