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(ed.). Gravitational waves (IOP, 2001)(422s).

(ed.). Gravitational waves (IOP, 2001)(422s).

(ed.). Gravitational waves (IOP, 2001)(422s).

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The relic graviton background 311Figure 16.8. Graviton spectra in the standard inflationary scenario.Figure 16.9. A minimal model of the pre-big bang background.(for power-inflation the bound is even stronger [31]).This bound applies to all models characteriz<strong>ed</strong> by a flat or decreasingspectrum. The bound can be evad<strong>ed</strong>, however, if the spectrum is growing, like inthe string cosmology context. To illustrate this point, let us consider the simplestclass of the so-call<strong>ed</strong> ‘minimal’ pre-big bang models, characteriz<strong>ed</strong> by threemain kinematic phases [32, 44]: an initial low-energy, dilaton-driven phase, aninterm<strong>ed</strong>iate high-energy ‘string’ phase, in which α ′ and loop corrections becomeimportant, and a final standard, radiation-dominat<strong>ed</strong> phase (see figure 16.9). Thetimescale η s marks the transition to the high-curvature phase, and the timescaleη 1 , characteriz<strong>ed</strong> by a final curvature of order one in string units, marks thetransition to the radiation-dominat<strong>ed</strong> cosmology.

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