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Geometry and Thermodynamics of Black Holes in Magnetic Fields ...

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Conserved Charge <strong>and</strong> Angular Momentum• These can be calculated most simply <strong>in</strong> the KK reduced 3Dlanguage. The physical charge is given by the Gaussian <strong>in</strong>tegral∫∫Q = 1∆φ∗F =4π S2 4π S 2 e−4ϕ ¯∗ ¯F ,= ∆φ ∫dψ = ∆φ [ ] θ=πψ = q(1 − 14π 4π4 q2 B 2 ) + 2amB .θ=0∆φ is the period <strong>of</strong> the azimuthal coord<strong>in</strong>ate φ, determ<strong>in</strong>edby requir<strong>in</strong>g no conical s<strong>in</strong>gularities at N <strong>and</strong> S poles <strong>of</strong> S 2 :]∆φ = 2π[1 + 3 2 q2 B 2 + 2aqmB 3 + (a 2 m 2 +16 1 q4 )B 4 .• For angular momentum, follow<strong>in</strong>g Wald, for every Kill<strong>in</strong>g vectorξ the Noether method gives a conserved chargeQ[ξ] = 116π∫S 2 ∗P , P = dξ + 4(ξµ A µ ) F .Tak<strong>in</strong>g the azimuthal Kill<strong>in</strong>g vector with ξ = ∂/∂ ˜φ, where˜φ = (2π/∆φ) φ has canonical 2π period, then as a 1-form,<strong>and</strong> <strong>in</strong> the 3D language, we have

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