Behavior of Friedmann-Robertson-Walker Cosmological Models in Scalar-Tensor Gravity

Shawn J. Kolitch
(touchngo@cosmic.physics.ucsb.edu)

Douglas M. Eardley
(doug@itp.ucsb.edu)

20 pages LaTeX and 4 figures (figures available by anonymous ftp at nsfitp.itp.ucsb.edu in directory /figures as file nsf-itp-94-45.ps)

Annals of Physics 241, 128-151 (1995). // NSF-ITP-94-45 // gr-qc/9405016.

We analyze solutions to Friedmann-Robertson-Walker cosmologies in Brans-Dicke theory, where a scalar field is coupled to gravity. Matter is modelled by a $\gamma$-law perfect fluid, including false-vacuum energy as a special case. Through a change of variables, we reduce the field equations from fourth order to second order, and they become equivalent to a two-dimensional dynamical system. We then analyze the entire solution space of this dynamical system, and find that many qualitative features of these cosmologies can be gleaned, including standard non-inflationary or extended inflationary expansion, but also including bifurcations of stable or unstable expansion or contraction, noninflationary vacuum-energy dominated models, and several varieties of ``coasting," ``bouncing," ``hesitating," and ``vacillating" universes. It is shown that inflationary dogma, which states that a universe with curvature and dominated by inflationary matter will always approach a corresponding flat-space solution at late times, does not hold in general for the scalar-tensor theory, but rather that the occurence of inflation depends upon the initial energy of the scalar field relative to the expansion rate. In the case of flat space ($k=0$), the dynamical system formalism generates some previously known exact power-law solutions.