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One of the most important geodesics in a black-hole spacetime is the marginally bound spherical orbit.
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See Fig. 2 of [ 6 ] for the characteristic form of the effective radial potential
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In obtaining the solution ( 25
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Note that one finds Δ ℓ = M ln ( 1 + 2 ) \Delta\ell=M\ln(1+\sqrt{2}) for the prograde equatorial geodesic with cos i = 1 \cos i=1 , in accord with the result of [ 2 ]
Cited in the paper.
Note that one finds L / M μ = 2 / cos i L/M\mu=2/\cos i for extremal black holes with ϵ ≡ 0 \epsilon\equiv 0 , in accord with the result of [ 7 ]
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It is worth emphasizing again that the effective inclination angle i i is a constant
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2013
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