scholarly journals Quantum evaporation of classical breathers

2019 ◽  
Vol 100 (4) ◽  
Author(s):  
Jan Ollé ◽  
Oriol Pujolàs ◽  
Tanmay Vachaspati ◽  
George Zahariade
Keyword(s):  
2016 ◽  
Vol 41 ◽  
pp. 1660127
Author(s):  
Irina Dymnikova ◽  
Anna Dobosz ◽  
Bożena Sołtysek

We present a regular spherically symmetric cosmological model of the Lemaitre class distinguished by the holographic principle as the thermodynamically stable end-point of quantum evaporation of the cosmological horizon. A source term in the Einstein equations connects smoothly two de Sitter vacua with different values of cosmological constant and corresponds to anisotropic vacuum dark fluid defined by symmetry of its stress-energy tensor which is invariant under the radial boosts. Global structure of space-time is the same as for the de Sitter space-time. Cosmological evolution goes from a big initial value of the cosmological constant towards its presently observed value.


2016 ◽  
Vol 185 (3-4) ◽  
pp. 209-219 ◽  
Author(s):  
S. Balibar
Keyword(s):  

1996 ◽  
Vol 46 (S1) ◽  
pp. 387-388
Author(s):  
J. R. Matthias ◽  
J. C. Inkson ◽  
M. B. Sobnack

1997 ◽  
Vol 12 (23) ◽  
pp. 4167-4198 ◽  
Author(s):  
Marina Gibilisco

In a previous work, I discussed the effect of the primordial black holes (PBH's) quantum evaporation on the reionization of the Universe at small redshifts (z ≤ 60): in principle, the photons emitted during the evaporation of such objects could drive a new ionization for the Universe after the recombination epoch; this reionization process should happen during the last stages of the PBH's life, when they totally evaporate and emit a lot of massive and massless particles. The critical mass of a black hole whose lifetime is equal to the present age of the Universe is ~ 4.4 × 1014 h-0.3 g: thus, PBH's having a mass M ~ 1014 g are the ideal candidates to induce a reionization at small redshifts. While in my previous study, I considered an exact blackbody photon emission spectrum, here I will adopt a more realistic one, taking into account the quarks and gluons jets emission through the contribution of a known fragmentation function. When the BH temperature rises above the QCD confinement scale, ΛQCD, one should expect an important contribution from quarks and gluons emission in the form of jets. In this paper I also improved my analysis by considering without any approximation the cooling effects in the plasma temperature evolution; as a result, I obtained a satisfactory "late and sudden" reionization process, characterized by a very well controlled rise of the plasma temperature: the plasma heating is not so high to induce a strong distortion of the CBR spectrum, in agreement with the recent FIRAS upper limit on the comptonization parameter, yc < 2.5 × 10-5.


2016 ◽  
Vol 94 (2) ◽  
Author(s):  
D. J. Papoular ◽  
L. P. Pitaevskii ◽  
S. Stringari

2006 ◽  
Vol 96 (3) ◽  
Author(s):  
Rituparno Goswami ◽  
Pankaj S. Joshi ◽  
Parampreet Singh

1990 ◽  
Vol 165-166 ◽  
pp. 493-494
Author(s):  
M.A.H. Tucker ◽  
A.F.G. Wyatt

1996 ◽  
Vol 46 (S1) ◽  
pp. 391-392 ◽  
Author(s):  
F. Dalfovo ◽  
L. Pitaevskii ◽  
S. Stringari

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