4.4 “End of Inflation” Mechanism 97 Fig. 4.11: Prediction of the model for $^{N}$∗ , with Γ$_{ϕ}$ ≪ H$_{T I}$ and n , g , $^{H}$∗ , Γ$_{ϕ}$ and λ values from Table 4.2. (A plot of Eq. (4.52), with m = m$_{0}$ and Γ= g $^{2}$m$_{0}$ .) Figs. 4.12–4.17, with the parameter values of Table 4.2. The predicted values of n$_{s}$ and n ′ s of the model for a thermal waterfall field mass of m$_{0}$ ∼ 10 3 GeV for all three $^{φ}$∗ Cases are the same to within at least four significant figures. They are also both insensitive to the value of m$_{ψ}$ within its allowed range. n$_{s}$ and n ′ s are shown in Table 4.6, with them both being within current observational bounds [40]. Table 4.6: Prediction for n$_{s}$ and n ′ s of the model with primordial inflation being Chaotic Inflation, with α =1 , Γ$_{ϕ}$ ≪ H$_{TI}$ , m$_{ψ}$ =10 − 2 GeV, m$_{0}$ ∼ 10 3 GeV and the parameter values from Table 4.2. Quantity Value n$_{s}$ ≈ 0 . 9645 n ′ s ≈ − 0 . 001259 10 2 10 4 10 ✄ 10 ☎ 10 10 m 0 ( GeV ) 20 40 N$_{*}$