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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> 9<br />

space is exp<strong>and</strong>ing according to the Friedmann–Lemaître model of General Relativity<br />

(Slipher, 1917; Hubble, 1929). Extrapolated into the past, these observations<br />

show that the Universe has exp<strong>and</strong>ed from a state in which all its matter<br />

<strong>and</strong> energy had immense temperatures <strong>and</strong> densities.<br />

In fact, in the very early Universe the temperatures <strong>and</strong> densities were so high<br />

that the photons <strong>and</strong> the great variety of relativistic particles were in thermodynamic<br />

equilibrium. When the mean thermal energy kT ≫ mc 2 , conservation of<br />

energy implies that every elementary particle of rest mass m can be converted<br />

into every other particle. Creation <strong>and</strong> annihilation of particle–antiparticle pairs<br />

<strong>and</strong> the interactions with other particles thus keep any particular type of particle<br />

of mass m in equilibrium (<strong>and</strong> in large numbers) above the energy mc 2 . As<br />

the average energy in the Universe decreased due to its expansion to a value less<br />

than the equivalent mass mc 2 , particles of mass m which had decayed or been<br />

annihilated could no longer be replaced. This point is known as the threshold for<br />

that particular particle. Cosmic evolution is thus characterized by a sequencial<br />

‘dying off’ of the various types of particles, beginning with the most massive.<br />

The temperature T or the average thermal energy kT in the radiation cosmos,<br />

can be written as a function of time as (e.g. Unsöld & Bascheck, 2002)<br />

1.5<br />

t[s] <br />

(T [1010 K])<br />

2 <br />

1<br />

2 , (37)<br />

(kT[MeV ])<br />

as long as t ≤ 2 × 10 6 years <strong>and</strong> leaving out of consideration the details of each<br />

types of relativistic particle.<br />

Before one Planck time (tP ∼ 10 −43 s) all the four fundamental forces were<br />

unified into a single force. This phase of the Universe is called the Planck Era.<br />

During this era the theory of General Relativity, which treats space–time as<br />

a continuum, would have to be replaced by a still lacking Quantum Theory of<br />

Gravity. Only at the end of this era, i.e., when the Universe was ∼ 10 −43 s old,<br />

gravity separated from the other three forces (e.g. Unsöld & Bascheck, 2002).<br />

The period 10 −43 s < t < 10 −35 s is is called the Gr<strong>and</strong> Unification Era.<br />

During this era the electromagnetic, strong <strong>and</strong> weak interactions are unified<br />

in a single force mediated by an hypothetical boson X, with mass (energy) of<br />

order 10 14 GeV, which converts leptons into quarks <strong>and</strong> vice versa. At this stage<br />

the Universe consists of a plasma composed of quarks, gluons, leptons, photons,<br />

bosons X as well as their respective antiparticles. They are all present in equal<br />

abundances <strong>and</strong> are continuoslly being interconverted due to mutual collisions<br />

(e.g. Unsöld & Bascheck, 2002).<br />

When the temperature of the Universe goes below 10 14 GeV it turns out<br />

that the decaying X bosons are no longer replaced by new X bosons. As a<br />

result, we have the strong–electroweak phase transition, i.e., the separation of<br />

the strong <strong>and</strong> EW interactions (e.g. Unsöld & Bascheck, 2002).<br />

In order to explain problems such as ‘flatness’, ‘horizon’ <strong>and</strong> ‘monopole’, the<br />

present paradigm makes use of an inflationary stage of expansion in the very<br />

early Universe (Section 1.3). During inflation the scale factor R(t) growns exponentially<br />

from an initial value Ri, corresponding to the instant ti ∼ 10 −35 s

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