Boosted Kerr Black Hole in the Presence of Plasma †



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(a) (b)
Figure 6. (a) Plot of vs. for (continuous line), (dashed line), and

2

e e e

2
(dot-dashed line). We used, rc = 10, sin χ = 1, and = 0.5. (b) Plot of vs.
for = 0.1 (continuous line), = 0.2 (dashed line), and (dot-dashed line). We used,

c
=10, , and = 0.5. Note the scale used for the deflection angle: each value is multiplied by 1e 5. Figures taken from Ref. [30].
Finally, we consider the deflection angle in the case of plasma in a galaxy cluster. Due to the large temperature of electrons in the cluster, the distribution can be considered as homogeneous. In this sense, it is possible to suppose a SIS distribution. Hence, the plasma density has the form [6]

. (36)
Therefore, after using Equation (29), the deflection angle has the form [30]

(37)
where we define = κmp , 0 = r0/M, = /M2 , and b = b/2M.
In Figure 7a,b we plot as a function of and , respectively. In In order to obtain these plots we considered the case [6]. According to Figure 7, differences in the deflection angle can be seen clearly for the PGC distribution when compared with the previous distributions. Furthermore, Figure 7b shows that the deflection angle increases due to the dragging and small values of . In Figure 7c, we show the behavior of a function of the impact parameter b for all distributions. Observ that values of for the PGC distribution are grater than the other two distributions. In the figure, it is also possibel to see the small difference between SIS and NSIS distributions for small values of



Figure 7. (a) Plot of PGC vs. for (continuous line), (dashed line), and (dot-dashed line). We used, , 0 , , s = 0.03, and /ω2 . (b) Plot of αˆPGC vs. Λ for = 0.1 (continuous line), Jr = 0.2 (dashed line), and (dot-dashed line). We used 0 , sin and /ω2 = 0.5. Note the scale used for the deflection angle: each value is multiplied by . (c) Plot of vs. for SIS (continuous line), NSIS (dashed line), and PGC (dot-dashed line). We used Λ = 0.1, c , and and /ω2 = and /ω2 = 0.5. For NSIS we use Λ = 1 since no difference from SIS was found. Figures taken from Ref. [30]



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