Primordial Black Holes and Cosmological Phase Transitions Report ...

Primordial Black Holes and Cosmological Phase Transitions Report ... Primordial Black Holes and Cosmological Phase Transitions Report ...

03.07.2013 Views

PBHs and Cosmological Phase Transitions 190 Table 46: The contribution to β from the QCD Crossover. In yellow we show the cases for which there is a non–negligible contribution to β from the QCD Crossover. For more details see Tables 41 and 42. nmax log10(t+/1s) 1.28 1.30 1.32 1.34 1.36 1.38 1.40 1.42 1.44 1.46 1.48 1.50 1.52 1.54 1.56 1.58 1.60 1.62 1.64 -11 R R R R -10 R R R -9 R R R -8 R R R R -7 R R R RC -6 R RC RC RC -5 RC RC RC RC Fig. 106d -4 RC RC RC RC RC RC Fig. 106a Fig. 104 -3 RC RC RC RC RC RC* Fig. 106e Fig. 105 -2 RC RC RC RC RCea RCea Fig. 106f -1 R R Rea RCea RCea RCea RCea 0 R Rea Rea Rea Rea Rea Rea Rea

PBHs and Cosmological Phase Transitions 191 log 10Βtk 0 -20 -40 -60 -80 n1.48, log 10t1s4 -8 -6 -4 -2 log10 tk 1 s Figure 104: The fraction of the universe going into PBHs in a universe with a running–tilt power spectrum when n+ =1.48 and t+ = 10 −4 s. The dark curve represents the radiation contribution and the maroon line the observational constraints. The other curves represent the contribution from the QCD phase transition: Crossover (green), Lattice Fit (magenta) and Bag Model (blue). The latter two models for the QCD transition are excluded, due to observational constraints. log 10Βtk 0 -2.5 -5 -7.5 -10 -12.5 -15 -17.5 n1.52, log 10t1s3 -7 -6 -5 -4 -3 -2 -1 0 log10 tk 1 s Figure 105: The fraction of the universe going into PBHs in a universe with a running–tilt power spectrum when n+ =1.52 and t+ = 10 −3 s (see Figure 104 for more details). Whatever the model adopted for the QCD transition this case must be excluded, due to observational constraints.

PBHs <strong>and</strong> <strong>Cosmological</strong> <strong>Phase</strong> <strong>Transitions</strong> 191<br />

log 10Βtk<br />

0<br />

-20<br />

-40<br />

-60<br />

-80<br />

n1.48, log 10t1s4<br />

-8 -6 -4 -2<br />

log10 tk<br />

<br />

1 s <br />

Figure 104: The fraction of the universe going into PBHs in a universe with a<br />

running–tilt power spectrum when n+ =1.48 <strong>and</strong> t+ = 10 −4 s. The dark curve<br />

represents the radiation contribution <strong>and</strong> the maroon line the observational<br />

constraints. The other curves represent the contribution from the QCD phase<br />

transition: Crossover (green), Lattice Fit (magenta) <strong>and</strong> Bag Model (blue). The<br />

latter two models for the QCD transition are excluded, due to observational<br />

constraints.<br />

log 10Βtk<br />

0<br />

-2.5<br />

-5<br />

-7.5<br />

-10<br />

-12.5<br />

-15<br />

-17.5<br />

n1.52, log 10t1s3<br />

-7 -6 -5 -4 -3 -2 -1 0<br />

log10 tk<br />

<br />

1 s <br />

Figure 105: The fraction of the universe going into PBHs in a universe with a<br />

running–tilt power spectrum when n+ =1.52 <strong>and</strong> t+ = 10 −3 s (see Figure 104<br />

for more details). Whatever the model adopted for the QCD transition this case<br />

must be excluded, due to observational constraints.

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