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The question of whether collider produced of subnuclear black holes might constitute a catastrophic risk is explored in a model of Casadio & Harms (2002) that treats them as quantum-mechanical objects. A plausible scenario in which these black holes accrete ambient matter at the Eddington limit shortly after their production, thereby emitting Hawking radiation that would be harmful to Earth and/or CERN and its surroundings, is described. Such black holes are shown to remain undetectable in existing astrophysical observations and thus evade a recent exclusion of risks from subnuclear black holes by Giddings & Mangano (2008) and and a similar one by Koch et al. (2009). I further question that these risk analyses are complete for the reason that they exclude plausible black-hole parameter ranges from safety consideration without giving any reason. Some feasible operational measures at colliders are proposed that would allow the lowering of any remaining risk probability. Giddings & Mangano drew different general conclusions only because they made different initial assumptions about the properties of microscopic black holes, not because any of their technical conclusions are incorrect. A critical comment by Giddings & Mangano (2008) on the present paper and a preprint by Casadio et al.(2009) - that presents a treatment of the present issue with methods and assumptions similar to mine - are addressed in appendices.
We calculate the Hawking temperature for a self-dual black hole in the context of quantum tunneling formalism.
Photon charge has been of interest as a phenomenological testing ground for basic assumptions in fundamental physics. There have been several constraints on the photon charge based on very different considerations. In this paper we put further limits
The relevant physics for the possible formation of black holes in the LHC is discussed.
A quantum equation of gravity is proposed using the geometrical quantization of general relativity. The quantum equation for a black hole is solved using the Wentzel-Kramers-Brillouin (WKB) method. Quantum effects of a Schwarzschild black hole are de
We examine the LHC phenomenology of quantum black holes in models of TeV gravity. By quantum black holes we mean black holes of the smallest masses and entropies, far from the semiclassical regime. These black holes are formed and decay over short di