We study the decay of the false vacuum in the regime where the quantum field theory analysis is not valid, since gravitational effects become important. This happens when the height of the barrier separating the false and the true vacuum is large, and it has implications for the instability of de Sitter, Minkowski and anti-de Sitter vacua. We carry out the calculations for a scalar field with a potential coupled to gravity, and work within the thin-wall approximation, where the bubble wall is thin compared to the size of the bubble. We show that the false de Sitter vacuum is unstable, independently of the height of the potential and the relative depth of the true vacuum compared to the false vacuum. The false Minkowski and anti-de Sitter vacua can be stable despite the existence of a lower energy true vacuum. However, when the relative depth of the true and false vacua exceeds a critical value, which depends on the potential of the false vacuum and the height of the barrier, then the false Minkowski and anti-de Sitter vacua become unstable. We calculate the probability for the decay of the false de Sitter, Minkowski and anti-de Sitter vacua, as a function of the parameters characterizing the field potential.
Click here to enter the meeting room 1.01, Pasteura 5 at 12:15

Daniele Perri (IFT UW)
Magnetic monopoles are intriguing hypothetical particles and inevitable predictions of theories of Grand Unification. They should be produced during phase transitions in the early universe, but mechanisms like the Schwinger effect in strong magnetic fields could also contribute to the monopole number density. I will show how we can infer additional bounds on the magnetic monopole flux from detecting intergalactic magnetic fields, and how even well-established limits, such as Parker bounds and limits from terrestrial experiments, strongly depend on the acceleration in cosmic magnetic fields. I will also discuss the implications of these bounds for minicharged monopoles and magnetic black holes as dark matter candidates. Finally, we apply our primordial bounds to monopoles produced by the primordial magnetic fields themselves through the Schwinger effect, deriving necessary conditions for the survival of the primordial fields.
join us at 12:15

Oleg Lebedev (Helsinki U.)
Non-thermal dark matter models suffer from the ever-presentgravitational particle production background, which marspredictivity of the framework altogether. I will discuss a classof freeze-in dark matter models with a low reheating temperaturethat are free of such problems and are directly testable.
Click here to enter the meeting room 1.01, Pasteura 5 at 12:15

Theodoros Papanikolaou (SSM & INFN Napoli)
Primordial black holes (PBHs) can generically form through the collapse of enhanced cosmological perturbations, constituting in some specific mass ranges a viable candidate for dark matter. Interestingly enough, the enhanced cosmological perturbations which collapse to form PBHs as well as the PBH energy density perturbations themselves can produce a stochastic gravitational-wave (GW) background induced by second-ordergravitational interactions, which can be detectable in GW observatories. In this talk, afterintroducing initially the motivation for the physics of PBHs and the associated to them GWsignals I will focus afterwards on the ultra-light PBH mass range and its induced GWsignatures through which one can probe the physics of the primordial Universe, theunderlying gravity theory testing as well fundamental high-energy physics theories.
room 1.01, Pasteura 5 at 12:15

Maxim Laletin (IFT UW)
Axions can be produced via the interactions in the thermal plasma of the early Universe and their contribution to dark radiation can modify the cosmological observables and constrain the axion couplings to SM particles. In my talk I am going to outline an approach to calculate the axion cosmological abundance that goes beyond the approximations widely used in the literature on the topic and demonstrate how it affects the bounds on axion couplings on the example of axion interactions with leptons.