Quantum mechanics of stationary states of particles in a space-time of classical black holes
arXiv:2012.04491 · doi:10.1134/S0040577920110070
Abstract
We consider interactions of scalar particles, photons, and fermions in Schwarzschild, Reissner-Nordström, Kerr, and Kerr-Newman gravitational and electromagnetic fields with a zero and nonzero cosmological constant. We also consider interactions of scalar particles, photons, and fermions with nonextremal rotating charged black holes in a minimal five-dimensional gauge supergravity. We analyze the behavior of effective potentials in second-order relativistic Schrödinger-type equations. In all cases, we establish the existence of the regime of particle "falling" on event horizons. An alternative can be collapsars with fermions in stationary bound states without a regime of particles "falling".
37 pages, 1 figure
References in corpus (5)
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- Maxwell's Equations in the Myers-Perry Geometry
- Stationary solutions of the second-order equation for fermions in Kerr-Newman space-time
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Cited by in corpus (7)
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- Quantization of spinor field in the Schwarzschild spacetime and spin sums for solutions of the Dirac equation
- The Quantum Model of Spinning Black Holes
- Something new about radial wave functions of fermions in the repulsive Coulomb field
- Prüfer transformation and its application to the numerical description of the motion of quantum particles with various spins in the fields of classical black holes
- Quantum probing of singularities at event horizons of black holes