cauchy integral
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2021 ◽  
Author(s):  
Wen-Xiang Chen

Abstract In this article, a new variable y is added here to expand the results of the above article.We use the properties of the Laurent series and the Cauchy integral. When y is greater than a certain limit, the effective potential of the equation does not have a pole, then there is no potential well outside the event horizon, when p 2(a 2 + Q2)/r2 + < ω < mΩH + qΦH,so the Kerr-Newman black hole is superradiantly stable at that time.


2021 ◽  
Author(s):  
Wen-Xiang Chen

Abstract In this article, a new variable y is added here to expand the results of the above article.We use the properties of the Laurent series and the Cauchy integral. When y is greater than a certain limit, the effective potential of the equation does not have a pole, then there is no potential well outside the event horizon, when p 2(a 2 + Q2)/r2 + < ω < mΩH + qΦH,so the Kerr-Newman black hole is superradiantly stable at that time.


2021 ◽  
Author(s):  
Wen-Xiang Chen

In this article, a new variable y is added here to expand the results of the above article.We use the properties of the Laurent series and the Cauchy integral. When y is greater than a certain limit, the effective potential of the equation does not have a pole, then there is no potential well outside the event horizon, when $\sqrt{2(a^2+Q^2)}/{r^2_+}&lt; \omega&lt; m\varOmega_H+q\varPhi_H$,so\ the Kerr-Newman black hole is superradiantly stable at that time.


2021 ◽  
Vol 93 (5) ◽  
Author(s):  
Johan Helsing ◽  
Andreas Rosén

AbstractA new integral equation formulation is presented for the Maxwell transmission problem in Lipschitz domains. It builds on the Cauchy integral for the Dirac equation, is free from false eigenwavenumbers for a wider range of permittivities than other known formulations, can be used for magnetic materials, is applicable in both two and three dimensions, and does not suffer from any low-frequency breakdown. Numerical results for the two-dimensional version of the formulation, including examples featuring surface plasmon waves, demonstrate competitiveness relative to state-of-the-art integral formulations that are constrained to two dimensions. However, our Dirac integral equation performs equally well in three dimensions, as demonstrated in a companion paper.


Author(s):  
V.L. Makarov ◽  
◽  
I.P. Gawriljuk ◽  
V.B. Vasylyk ◽  
◽  
...  

A homogeneous fractional-differential equation with a fractional Hardy—Titchmarsh integral and an unboun-ded operator coefficient in a Banach space is considered. The conditions for the representation of the solution in the form of a Danford—Cauchy integral are established, and an exponentially convergent approximation method is developed.


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