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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> 131<br />

∆<br />

1.4<br />

1.2<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

x2 x15 x30 x90<br />

∆c2<br />

∆c1 ∆c2<br />

∆c1<br />

No BH formation<br />

BH formation<br />

BH formation<br />

No BH formation<br />

∆c0.7<br />

∆c13<br />

20 40 60 80 100<br />

x<br />

Figure 54: The curve in the (x, δ) plane indicating which parameter values lead<br />

to collapse to a BH, within the QCD Bag Model, in the case x>1 with δc =1/3<br />

<strong>and</strong> δc =0.7. We show the values of x corresponding to the cases presented in<br />

Figures 50, 51 <strong>and</strong> 53. The intersection point δc1 = δc2 occurs for x ≈ 54.8 when<br />

δc =1/3 <strong>and</strong> x ≈ 13.6 when δc =0.7. The intersection point δc2 = δc =1/3<br />

occurs for x ≈ 12.0 when δc =1/3 <strong>and</strong> x ≈ 3.5 when δc =0.7.<br />

x<br />

50<br />

40<br />

30<br />

20<br />

10<br />

∆c2∆c<br />

∆c1∆c2<br />

0.35 0.4 0.45 0.5 0.55 0.6 0.65 0.7<br />

Figure 55: The value of x as a function of δc for the special cases δc1 = δc2<br />

<strong>and</strong> δc2 = δc for the QCD phase transition according to the Bag Model. The<br />

dots represent the values obtained numerically (see Table 28) <strong>and</strong> the solid lines<br />

represent the cubic interpolations (equations 259 <strong>and</strong> 260).<br />

∆c

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