Conditions for the cosmological viability of f(R) dark energy models

被引:642
作者
Amendola, Luca
Gannouji, Radouane
Polarski, David
Tsujikawa, Shinji
机构
[1] Osserv Astron Roma, INAF, I-00040 Monte Porzio Catone, Roma, Italy
[2] Univ Montpellier 2, LPTA, CNRS, F-34095 Montpellier 05, France
[3] Gunma Natl Coll Technol, Dept Phys, Gunma 3718530, Japan
来源
PHYSICAL REVIEW D | 2007年 / 75卷 / 08期
关键词
D O I
10.1103/PhysRevD.75.083504
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We derive the conditions under which dark energy models whose Lagrangian densities f are written in terms of the Ricci scalar R are cosmologically viable. We show that the cosmological behavior of f(R) models can be understood by a geometrical approach consisting of studying the m(r) curve on the (r,m) plane, where m equivalent to Rf(,RR)/f(,R) and r equivalent to -Rf(,R)/f with f(,R)equivalent to df/dR. This allows us to classify the f(R) models into four general classes, depending on the existence of a standard matter epoch and on the final accelerated stage. The existence of a viable matter-dominated epoch prior to a late-time acceleration requires that the variable m satisfies the conditions m(r) approximate to + 0 and dm/dr > -1 at r approximate to -1. For the existence of a viable late-time acceleration we require instead either (i) m = -r -1, (root 3 -1 ) /2 < m <= 1 and dm/dr < - 1 or (ii) 0 < m <= 1 at r = -2. These conditions identify two regions in the (r,m) space, one for the matter era and the other for the acceleration. Only models with an m(r) curve that connects these regions and satisfies the requirements above lead to an acceptable cosmology. The models of type f(R)= alpha R-n and f = R+alpha R-n do not satisfy these conditions for any n > 0 and n < -1 and are thus cosmologically unacceptable. Similar conclusions can be reached for many other examples discussed in the text. In most cases the standard matter era is replaced by a cosmic expansion with scale factor a proportional to t(1/2). We also find that f(R) models can have a strongly phantom attractor but in this case there is no acceptable matter era.
引用
收藏
页数:22
相关论文
共 120 条
[1]  
ABDALLA MCB, HEPTH0601213
[2]   Is there supernova evidence for dark energy metamorphosis? [J].
Alam, U ;
Sahni, V ;
Saini, TD ;
Starobinsky, AA .
MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY, 2004, 354 (01) :275-291
[3]  
ALLEMANDI G, 2004, PHYS REV D, V707, P3503
[4]   Tracking and coupled dark energy as seen by the Wilkinson Microwave Anisotropy Probe [J].
Amendola, L ;
Quercellini, C .
PHYSICAL REVIEW D, 2003, 68 (02)
[5]   Stationary dark energy: The present universe as a global attractor [J].
Amendola, L ;
Tocchini-Valentini, D .
PHYSICAL REVIEW D, 2001, 64 (04) :5
[6]   Scaling solutions in general nonminimal coupling theories [J].
Amendola, L .
PHYSICAL REVIEW D, 1999, 60 (04)
[7]   Coupled quintessence [J].
Amendola, L .
PHYSICAL REVIEW D, 2000, 62 (04) :10
[8]  
AMENDOLA L, ASTROPH0605384
[9]   Are f(R) dark energy models cosmologically viable? [J].
Amendola, Luca ;
Polarski, David ;
Tsujikawa, Shinji .
PHYSICAL REVIEW LETTERS, 2007, 98 (13)
[10]   Challenges for scaling cosmologies [J].
Amendola, Luca ;
Quartin, Miguel ;
Tsujikawa, Shinji ;
Waga, Ioav .
PHYSICAL REVIEW D, 2006, 74 (02)