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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> xiii<br />

29 The values of δAB, δBC, δc1 <strong>and</strong> δc2 for different values of x (when<br />

x>1) <strong>and</strong> δc according to the QCD Bag Model . . . . . . . . . . 128<br />

30 The values of δBC, δCE <strong>and</strong> δc1 for different values of x (when<br />

y −1 < x < 1) <strong>and</strong> δc according to the QCD Bag Model . . . . . . 135<br />

31 The values of δEF <strong>and</strong> δc1 for different values of x (when x < y −1 )<br />

<strong>and</strong> δc according to the QCD Bag Model . . . . . . . . . . . . . . 139<br />

32 The evolution of δc1 <strong>and</strong> δc2 as functions of time <strong>and</strong> as functions<br />

of the parameter x for the QCD Bag Model . . . . . . . . . . . . 142<br />

33 The evolution of δc1 as a function of time for the QCD Crossover 146<br />

34 The evolution of δcA, δc1 <strong>and</strong> δc2 as a function of time for the<br />

QCD Lattice Fit . . . . . . . . . . . . . . . . . . . . . . . . . . . 157<br />

35 The lowest value of δc1,min for the EW Crossover with δc assuming<br />

different values . . . . . . . . . . . . . . . . . . . . . . . . . . 160<br />

36 The evolution of δc1 as a function of time for a EW Crossover<br />

with ∆T =0.013Tc when δc =1/3 . . . . . . . . . . . . . . . . . 164<br />

37 The evolution of δc1 <strong>and</strong> δc2 as functions of time <strong>and</strong> as functions<br />

of the parameter x for the EW Bag Model when δc =1/3 . . . . 166<br />

38 The evolution of δc1 for the cosmological electron–positron annihilation<br />

with ∆T =0.115Tc <strong>and</strong> δc =1/3 . . . . . . . . . . . . . 169<br />

39 The values of n2 <strong>and</strong> n3 when nmax =1.4 . . . . . . . . . . . . . 173<br />

40 The different scenarios concerning the calculus of β . . . . . . . . 175<br />

41 Different contributions to β . . . . . . . . . . . . . . . . . . . . . 177<br />

42 The cases for which β> 10 −100 for a radiation–dominated Universe<br />

with a running–tilt power law spectrum . . . . . . . . . . . 181<br />

43 The contribution to β from the electron–positron annihilation<br />

epoch . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 184<br />

44 The contribution to β from the QCD Bag Model . . . . . . . . . 188<br />

45 The contribution to β from the QCD Lattice Fit . . . . . . . . . 189<br />

46 The contribution to β from the QCD Crossover . . . . . . . . . . 190<br />

47 The contribution to β from the EW Bag Model . . . . . . . . . . 194<br />

48 Peaks of the curve β(tk) in the case n+ =1.36 <strong>and</strong> t+ = 10 −7 s . 199<br />

49 The fraction of the universe going into PBHs during radiation<br />

domination <strong>and</strong> during cosmological phase transitions (the value<br />

of βmax for the various contributions) . . . . . . . . . . . . . . . 201<br />

50 The ten cases with the largest contribution from the QCD Crossover<br />

to β(tk) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 210<br />

51 The ten cases with the largest contribution from the QCD Bag<br />

Model to β(tk) . . . . . . . . . . . . . . . . . . . . . . . . . . . . 211<br />

52 The ten cases with the largest contribution from the QCD Lattice<br />

Fit to β(tk) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 212<br />

53 The ten cases with the largest contribution from the EW Bag<br />

Model to β(tk) . . . . . . . . . . . . . . . . . . . . . . . . . . . . 214<br />

54 The ten cases with the largest contribution from the electron–<br />

positron annihilation epoch to β(tk) . . . . . . . . . . . . . . . . 215

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