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The today's energy density of the induced (second order) gravitational wave background in the frequency region $\sim 10^{-3} - 10^3$ Hz is constrained using the existing limits on primordial black hole production in the early Universe. It…

Cosmology and Nongalactic Astrophysics · Physics 2014-11-20 Edgar Bugaev , Peter Klimai

We study the linear polarization of the accretion disk around black holes with a dark matter halo. The interaction of the black hole with the dark matter is modelled by considering an exact solution to the Einstein equations which describes…

General Relativity and Quantum Cosmology · Physics 2025-03-28 Tsanimir Angelov , Rasim Bekir , Galin Gyulchev , Petya Nedkova , Stoytcho Yazadjiev

The mild form of the Weak Gravity Conjecture states that quantum or higher-derivative corrections should decrease the mass of large extremal charged black holes at fixed charge. This allows extremal black holes to decay, unless protected by…

High Energy Physics - Theory · Physics 2021-04-27 Lars Aalsma , Alex Cole , Gregory J. Loges , Gary Shiu

In supersymmetric theories the mass of any state is bounded below by the values of some of its charges. The corresponding bounds in case of Schwarzschild and Reissner-Nordstr\"om black holes are known to coincide with the requirement that…

High Energy Physics - Theory · Physics 2009-09-29 Renata Kallosh , Andrei Linde , Tomás Ortín , Amanda Peet , Antoine Van Proeyen

Axions, grand unification, and string theory are each compelling extensions of the Standard Model. We show that combining these frameworks imposes strong constraints on the QCD axion mass. Using unitarity arguments and explicit string…

High Energy Physics - Phenomenology · Physics 2025-05-23 Joshua N. Benabou , Katherine Fraser , Mario Reig , Benjamin R. Safdi

In order to accommodate increasingly tighter observational constraints on dark matter, several models have been proposed recently in which dark matter particles are charged under some hidden gauge group. Hidden gauge charges are invisible…

High Energy Physics - Phenomenology · Physics 2009-12-04 De-Chang Dai , Katherine Freese , Dejan Stojkovic

The invariant four-volume $\mathcal{V}$ of a complete black hole (the volume of the spacetime at and interior to the horizon) diverges. However, if one considers the black hole set up by the gravitational collapse of an object, and…

General Relativity and Quantum Cosmology · Physics 2010-06-03 William Ballik , Kayll Lake

We study the formation of primordial black holes (PBHs) from density fluctuations due to supercooled phase transitions (PTs) triggered in an axion-like particle (ALP) model. We find that the mass of the PBHs is inversely correlated with the…

Cosmology and Nongalactic Astrophysics · Physics 2025-10-02 Angela Conaci , Luigi Delle Rose , P. S. Bhupal Dev , Anish Ghoshal

Nearly massless axion-like particles are of interest for astrophysical observations, and some constraints on their parameter space do exist in the literature. Here, we propose to put new constraints on these particles using polarisation…

Cosmology and Nongalactic Astrophysics · Physics 2012-05-01 A. Payez , J. R. Cudell , D. Hutsemékers

Static black holes of dilaton-axion gravity become singular in the extreme limit, which prevents a direct determination of their near-horizon geometry. This is addressed by first taking the near-horizon limit of extreme rotating NUT-less…

General Relativity and Quantum Cosmology · Physics 2017-08-23 G. Clement , D. Gal'tsov

In this thesis, we explore the possibility to define black hole mass in terms of the Weyl tensor for the entire family of Lovelock-AdS gravity theories. The level of degeneracy $k$ of the corresponding vacuum fixes the number of curvatures…

High Energy Physics - Theory · Physics 2020-02-13 Gabriel Arenas-Henriquez

In this essay it is proved that there are black holes that are dangerously cold. In particular, by analyzing the emission spectra of highly charged black holes we reveal the fact that near-extremal black holes whose Bekenstein-Hawking…

General Relativity and Quantum Cosmology · Physics 2023-12-20 Shahar Hod

In this paper, with considering the nonlinear electromagnetic field coupled to Einstein gravity, we obtain the higher dimensional slowly rotating charged black hole solutions. By use of the fact that the temperature of the extreme black…

High Energy Physics - Theory · Physics 2010-11-15 S. H. Hendi

This paper puts forward a conjecture that there are no black holes in M theory. We will show that a mechanism to prevent black hole formation is needed in 4 dimensions to make string theory a viable high energy model of quantum gravity.…

High Energy Physics - Theory · Physics 2016-06-07 Michael Hewitt

Massless black holes can be understood as bound states of a (positive mass) extreme a=\sqrt{3} black hole and a singular object with opposite (i.e. negative) mass with vanishing ADM (total) mass but non-vanishing gravitational field.…

High Energy Physics - Theory · Physics 2016-08-24 Tomas Ortin

We derive a general formula for the center-of-mass (CM) energy for the near-horizon collision of two particles of the same rest mass on the equatorial plane around a Kerr black hole. We then apply this formula to a particle which plunges…

General Relativity and Quantum Cosmology · Physics 2011-10-21 Tomohiro Harada , Masashi Kimura

Gamma-rays are, with antiprotons, a very efficient way to derive upper limits on the density of evaporating black holes. They have been successfully used in the last decades to severely constrain the amount of Primordial Black Holes (PBHs)…

Astrophysics · Physics 2007-05-23 A. Barrau , G. Boudoul , L. Derome

The observed values of the cosmological constant {\it and} the abundance of Dark Matter (DM) can be successfully understood, using certain measures, by imposing the anthropic requirement that density perturbations go non-linear and…

High Energy Physics - Phenomenology · Physics 2015-03-13 Francesco D'Eramo , Lawrence J. Hall , Duccio Pappadopulo

A new theorem for black holes is found. It is called the horizon mass theorem. The horizon mass is the mass which cannot escape from the horizon of a black hole. For all black holes: neutral, charged or rotating, the horizon mass is always…

General Relativity and Quantum Cosmology · Physics 2015-06-25 Yuan K. Ha

The generalization of the black hole in three-dimensional spacetime to include an electric charge Q in addition to the mass M and the angular momentum J is given. The field equations are first solved explicitly when Q is small and the…

High Energy Physics - Theory · Physics 2009-10-31 Cristian Martinez , Claudio Teitelboim , Jorge Zanelli