TY - JOUR
T1 - Coupled dark energy
T2 - Towards a general description of the dynamics
AU - Gumjudpai, Burin
AU - Naskar, Tapan
AU - Sami, M.
AU - Tsujikawa, Shinji
PY - 2005/6/1
Y1 - 2005/6/1
N2 - In dark energy models of scalar-field coupled to a barotropic perfect fluid, the existence of cosmological scaling solutions restricts the Lagrangian of the field φ to p ≤ Xg(Xeλφ), where , λ is a constant and g is an arbitrary function. We derive general evolution equations in an autonomous form for this Lagrangian and investigate the stability of fixed points for several different dark energy models: (i) ordinary (phantom) field, (ii) dilatonic ghost condensate, and (iii) (phantom) tachyon. We find the existence of scalar-field dominant fixed points (Ω φ ≤ 1) with an accelerated expansion in all models irrespective of the presence of the coupling Q between dark energy and dark matter. These fixed points are always classically stable for a phantom field, implying that the universe is eventually dominated by the energy density of a scalar field if a phantom is responsible for dark energy. When the equation of state wφ for the field φ is larger than -1, we find that scaling solutions are stable if the scalar-field dominant solution is unstable, and vice versa. Therefore in this case the final attractor is either a scaling solution with constant Ωφ satisfying 0 < Ωφ < 1 or a scalar-field dominant solution with Ωφ ≤ 1.
AB - In dark energy models of scalar-field coupled to a barotropic perfect fluid, the existence of cosmological scaling solutions restricts the Lagrangian of the field φ to p ≤ Xg(Xeλφ), where , λ is a constant and g is an arbitrary function. We derive general evolution equations in an autonomous form for this Lagrangian and investigate the stability of fixed points for several different dark energy models: (i) ordinary (phantom) field, (ii) dilatonic ghost condensate, and (iii) (phantom) tachyon. We find the existence of scalar-field dominant fixed points (Ω φ ≤ 1) with an accelerated expansion in all models irrespective of the presence of the coupling Q between dark energy and dark matter. These fixed points are always classically stable for a phantom field, implying that the universe is eventually dominated by the energy density of a scalar field if a phantom is responsible for dark energy. When the equation of state wφ for the field φ is larger than -1, we find that scaling solutions are stable if the scalar-field dominant solution is unstable, and vice versa. Therefore in this case the final attractor is either a scaling solution with constant Ωφ satisfying 0 < Ωφ < 1 or a scalar-field dominant solution with Ωφ ≤ 1.
KW - Dark energy theory
KW - String theory and cosmology
UR - http://www.scopus.com/inward/record.url?scp=22144488834&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=22144488834&partnerID=8YFLogxK
U2 - 10.1088/1475-7516/2005/06/007
DO - 10.1088/1475-7516/2005/06/007
M3 - Article
AN - SCOPUS:22144488834
SP - 101
EP - 129
JO - Journal of Cosmology and Astroparticle Physics
JF - Journal of Cosmology and Astroparticle Physics
SN - 1475-7516
IS - 6
ER -