Manipulation of Fluxoid by Electromagnetic Perturbation

2014 ◽  
Vol 2 ◽  
pp. 34-37
Author(s):  
Takashi HIKIHARA ◽  
Yohei HOSOE ◽  
Tomomichi HAGIWARA
2019 ◽  
Vol 100 (21) ◽  
Author(s):  
Surajit Dutta ◽  
Indranil Roy ◽  
Soumyajit Mandal ◽  
John Jesudasan ◽  
Vivas Bagwe ◽  
...  

2002 ◽  
Vol 17 (20) ◽  
pp. 2752-2752
Author(s):  
VITOR CARDOSO ◽  
JOSÉ P. S. LEMOS

We studied the quasi-normal modes (QNM) of electromagnetic and gravitational perturbations of a Schwarzschild black hole in an asymptotically anti-de Sitter (AdS) spacetime, extending previous works1,2 on the subject. Some of the electromagnetic modes do not oscillate, they only decay, since they have pure imaginary frequencies. The gravitational modes show peculiar features: the odd and even gravitational perturbations no longer have the same characteristic quasinormal frequencies. There is a special mode for odd perturbations whose behavior differs completely from the usual one in scalar1 and electromagnetic perturbation in an AdS spacetime, but has a similar behavior to the Schwarzschild black hole3 in an asymptotically flat spacetime: the imaginary part of the frequency goes as [Formula: see text], where r+ is the horizon radius. We also investigated the small black hole limit showing that the imaginary part of the frequency goes as [Formula: see text]. These results are important to the AdS/CFT4 conjecture since according to it the QNMs describe the approach to equilibrium in the conformal field theory. For other geometries see5,6.


1995 ◽  
Vol 54 (1) ◽  
pp. 31-58 ◽  
Author(s):  
D. van Eester

A semi-analytical approach is proposed for computing the non-local response of a toroidal plasma to an electromagnetic perturbation. Although the perturbed distribution function as well as the absorbed power are also computed, the focus is on the associated quasi-linear diffusion operator. Different decorrelation models allow one to recapture the well-known ideal collisionless plasma result where the wave–particle energy exchange is exactly at resonance, as well as the more realistic plasma response where the interaction region is widened. The choice of the independent variables also allows one to carry out all computations except the integration of the guiding-centre motion analytically.


1991 ◽  
Vol 69 (11) ◽  
pp. 7735-7739 ◽  
Author(s):  
L. Lanotte ◽  
C. Luponio ◽  
F. Porreca

2015 ◽  
Vol 62 (3) ◽  
pp. 1383-1394 ◽  
Author(s):  
M. Ribiere ◽  
S. Demarquay ◽  
M. Maulois ◽  
R. Maisonny ◽  
T. DaAlmeida ◽  
...  

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