Revisiting Primordial Black Hole Evolution

被引:4
作者
Khlopov, Maxim [1 ,2 ,3 ]
Paik, Biplab [4 ,5 ]
Ray, Saibal [5 ]
机构
[1] Natl Res Nucl Univ MEPhI, Moscow Engn Phys Inst, Moscow 115409, Russia
[2] Univ Paris, Astroparticule & Cosmol, CNRS, F-75013 Paris, France
[3] Southern Fed Univ, Inst Phys, Stachki 194, Rostov Na Donu 344090, Russia
[4] Rautara MNM High Sch, North 24, Parganas 743234, W Bengal, India
[5] Govt Coll Engn & Ceram Technol, Dept Phys, Kolkata 700010, W Bengal, India
关键词
cosmology; particle physics; primordial black hole; baryon accretion; forbidden regime; high energy physics; PARTICLE-EMISSION RATES; SELF-SIMILAR GROWTH; COSMIC-RAYS; SPHERICAL ACCRETION; MASSLESS PARTICLES; CONSTRAINTS; MODULATION; RADIATION; REMNANTS; DENSITY;
D O I
10.3390/axioms9020071
中图分类号
O29 [应用数学];
学科分类号
070104 ;
摘要
Primordial black holes (PBHs) are the sensitive probe for physics and cosmology of very early Universe. The observable effect of their existence depends on the PBH mass. Mini PBHs evaporate and do not survive to the present time, leaving only background effect of products of their evaporation, while PBHs evaporating now can be new exotic sources of energetic particles and gamma rays in the modern Universe. Here we revisit the history of evolution of mini PBHs. We follow the aspects associated withgrowth versus evaporation rateof "a mini PBH being trapped inside intense local cosmological matter inhomogeneity". We show that the existence of baryon accretion forbidden black hole regime enables constraints on mini PBHs with the mass M <= 5.5 x 10(13) g. On the other hand, we propose the mechanism of delay of evaporation of primordial population of PBHs of primordial mass range 5.5 x 10(13) g <= M <= 5.1 x 10(14) g. It can provide their evaporation to be the main contributor to gamma-ray flux distribution in the current Universe. At the final stage of evaporation these PBHs can be the source of ultrahigh energy cosmic rays and gamma radiation challenging probe for their existence in the LHAASO experiment.
引用
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页数:24
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