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Primordial Black Holes and Cosmological Phase Transitions Report ...

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PBHs <strong>and</strong> <strong>Cosmological</strong> <strong>Phase</strong> <strong>Transitions</strong> 199<br />

Table 48: Peaks of the curve β(tk) in the case n+ =1.36 <strong>and</strong> t+ = 10 −7 s. See<br />

Table 40 for the description of different scenarios.<br />

Scenario Number Description Figure<br />

of peaks<br />

1 2 Radiation + QCD Bag Model 110a<br />

2 2 Radiation + QCD Lattice Fit 110b<br />

3 1 Radiation 110c<br />

4 3 Radiation + EW Bag Model + QCD Bag Model 110d<br />

5 3 Radiation + EW Bag Model + QCD Lattice Fit 110e<br />

6 2 Radiation + EW Bag Model 110f<br />

When n+ =1.22 <strong>and</strong> n+ =1.24 there are a few cases for which the peak<br />

from the radiation contribution occurs for tk < 10 −23 s. Taking into account<br />

that our expression for β(tk) is classic (Section 5.1), not valid for epochs earlier<br />

than ∼ 10 −23 s where the maximum is attained, we consider, for these particular<br />

cases, the values correspondent to tk = 10 −23 s (which correspond to<br />

PBHs exploding right now), <strong>and</strong> we show those values in Table 49 inside square<br />

brackets.<br />

For the QCD Crossover <strong>and</strong> for the electron–positron annihilation there are<br />

a lot of cases for which there is an important contribution to β, similar to the<br />

radiation contribution, but without any peak. As an example of this, we mention<br />

the case n+ =1.68 <strong>and</strong> t+ = 100 s (Figure 101f) for which we have a single<br />

peak from the radiation contribution. These cases are labeled, in Table 49, with<br />

‘NA’ (meaning Not Applicable).

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