Integral Equations of Fields on the Rotating Black Hole
Takahiro Masuda, Hisao Suzuki
Abstract
It is known that the radial equation of the massless fields with spin around Kerr black holes cannot be solved by special functions. Recently, the analytic solution was obtained by use of the expansion in terms of the special functions and various astrophysical application have been discussed. It was pointed out that the coefficients of the expansion by the confluent hypergeometric functions are identical to those of the expansion by the hypergeometric functions. We explain the reason of this fact by using the integral equations of the radial equation. It is shown that the kernel of the equation can be written by the product of confluent hypergeometric functions. The integral equaton transforms the expansion in terms of the confluent hypergeometric functions to that of the hypergeometric functions and vice versa,which explains the reason why the expansion coefficients are universal.
Create a lesson
Related papers
Instabilities of Simpson-Visser black bounces sourced by a phantom scalar and nonlinear electrodynamics
Kirill A. Bronnikov, Rustam Ibadov, Jutta Kunz
Parity-violating scalar-tensor theory revisited: complete basis up to d=4 and Hamiltonian analysis
Yun-Chuan Zhang, Yu-Min Hu, Xian Gao
A Smoothly Truncated Dark Matter Spike around a Black Hole in an Einstein-Cluster Model
Hassan Hassanabadi, Soroush Zare
Can ns hint at a parity-odd sector of gravity?
Christian Dioguardi
An Orbital Curvature for ISCOs
Poulami Mukherjee, Chandrasekhar Bhamidipati, Sudipta Mukherji
Gravitational Thermodynamicization of Primordial Black Holes: An RVB Residue Formulation of Thermal Formation and Nonequilibrium Evolution
Wen-Xiang Chen