An accelerating cosmology without dark energy

被引:81
作者
Steigman, G. [1 ]
Santos, R. C. [2 ]
Lima, J. A. S. [2 ]
机构
[1] Ohio State Univ, Dept Phys, Columbus, OH 43210 USA
[2] Univ Sao Paulo, Dept Astron, BR-05508900 Sao Paulo, Brazil
来源
JOURNAL OF COSMOLOGY AND ASTROPARTICLE PHYSICS | 2009年 / 06期
基金
巴西圣保罗研究基金会;
关键词
cosmology of theories beyond the SM; dark energy theory; CMBR theory; PARTICLE CREATION; QUANTIZED-FIELDS; CONSTRAINTS; THERMODYNAMICS; SUPERNOVAE; CONSTANT; LAMBDA;
D O I
10.1088/1475-7516/2009/06/033
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
The negative pressure accompanying gravitationally-induced particle creation can lead to a cold dark matter (CDM) dominated, accelerating Universe (Lima et al. 1996 [1]) without requiring the presence of dark energy or a cosmological constant. In a recent study, Lima et al. 2008 [2] (LSS) demonstrated that particle creation driven cosmological models are capable of accounting for the SNIa observations [3] of the recent transition from a decelerating to an accelerating Universe, without the need for Dark Energy. Here we consider a class of such models where the particle creation rate is assumed to be of the form Gamma = beta H + gamma H-0, where H is the Hubble parameter and H-0 is its present value. The evolution of such models is tested at low redshift by the latest SNe Ia data provided by the Union compilation [4] and at high redshift using the value of z(eq), the redshift of the epoch of matter - radiation equality, inferred from the WMAP constraints on the early Integrated Sachs-Wolfe (ISW) effect [5]. Since the contributions of baryons and radiation were ignored in the work of LSS, we include them in our study of this class of models. The parameters of these more realistic models with continuous creation of CDM are constrained at widely-separated epochs (z(eq) approximate to 3000 and z approximate to 0) in the evolution of the Universe. The comparison of the parameter values, {beta, gamma}, determined at these different epochs reveals a tension between the values favored by the high redshift CMB constraint on z(eq) from the ISW and those which follow from the low redshift SNIa data, posing a potential challenge to this class of models. While for beta = 0 this conflict is only at less than or similar to 2 sigma, it worsens as beta increases from zero.
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