Figure 11

Figure 11: Ratio of fluctuations before (Δ −) and after (Δ+) the bounce in the form |1 − Δ ∕Δ | − + as a function of a state parameter A in relation to the Hamiltonian H = ⟨ ˆH ⟩ for H = 1000 in Planck units. For larger H, the curve becomes even steeper, showing how precisely one has to tune the state parameter A in order to have a near symmetric state with |1 − Δ − ∕Δ+ | = 0. See [74] for further details.