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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> 156<br />

∆<br />

1.2<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

No BH formation<br />

BH formation<br />

∆cA<br />

No BH formation<br />

∆c2<br />

∆c1<br />

t t<br />

-9 -8 -7 -6 -5 -4 -3<br />

Log 10tk1s<br />

Figure 80: The curve in the (log 10(tk/1s), δ) plane indicating which parameter<br />

values lead to collapse to a BH in the case of the QCD Lattice Fit when δc =1/3.<br />

The vertical dashed lines correspond to tk = t− <strong>and</strong> tk = t+.<br />

7.3.4 Summary<br />

We now compile the results obtained on sections 7.3.1–7.3.3. We have determined<br />

the threshold δc for the entire QCD phase transition according to the<br />

Lattice Fit model. As a result we obtain Figure 80 for the case δc =1/3 <strong>and</strong><br />

Figure 81 for the case δc =0.7.<br />

During the QCD transition, the threshold for PBH formation (δc) experiences<br />

a reduction. As a result, a new window for PBH formation (between δc1<br />

<strong>and</strong> δc, between δcA <strong>and</strong> δc or between δc1 <strong>and</strong> δc2) is opened for a brief period.<br />

Note that the window between δcA <strong>and</strong> δc does not exist for the Bag Model<br />

case (Section 7.1.4) because, in that case, we have fA = 0. On Table 34 we<br />

present some values for this new threshold for PBH formation during the QCD<br />

transition according to the Lattice Fit, when δc =1/3.

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