Geometry and Thermodynamics of Black Holes in Magnetic Fields ...
Geometry and Thermodynamics of Black Holes in Magnetic Fields ...
Geometry and Thermodynamics of Black Holes in Magnetic Fields ...
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Rotat<strong>in</strong>g Generalisations?• Rotat<strong>in</strong>g generalisations have been obta<strong>in</strong>ed before. The solutionsare too complicated to work with reliably by h<strong>and</strong>,so it is useful first to reconstruct from scratch, us<strong>in</strong>g algebraiccomput<strong>in</strong>g. We used a solution-generat<strong>in</strong>g techniqueto “magnetise” Kerr-Newman, via a Kaluza-Kle<strong>in</strong> reductionto three dimensions. The start<strong>in</strong>g po<strong>in</strong>t is E<strong>in</strong>ste<strong>in</strong>-Maxwelltheory <strong>in</strong> four dimensions:L 4 = R − F 2 .We then assume a metric with a spacelike Kill<strong>in</strong>g vector ∂/∂φ<strong>and</strong> reduce to three dimensions:ds 2 4 = e2ϕ d¯s 2 3 + e−2ϕ (dφ + 2Ā) 2 ,A = Ā + χ (dφ + 2Ā) .This gives the three-dimensional Lagrangian¯L 3 = ¯R − 2(∂ϕ) 2 − 2e ϕ (∂χ) 2 − e −4ϕ ¯F 2 − e −2ϕ ¯F 2 ,where ¯F = dĀ <strong>and</strong> ¯F = dĀ + 2χ dĀ.• Dualis<strong>in</strong>g Ā <strong>and</strong> Ā; e −2ϕ ¯∗ ¯F = dψ <strong>and</strong> e −4ϕ ¯∗ ¯F = dσ − 2χ dψgives 3D gravity coupled to a nonl<strong>in</strong>ear sigma model:L 3 = ¯R − 2(∂ϕ) 2 − 2e ϕ [(∂χ) 2 + (∂ψ) 2 ] − 2e 2ϕ (∂σ − 2χ∂ψ) 2 .