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We investigate the instability of the massive scalar field in the vicinity of a rotating black hole. The instability arises from amplification caused by the classical superradiance effect. The instability affects bound states: solutions to the massive Klein-Gordon equation which tend to zero at infinity. We calculate the spectrum of bound state frequencies on the Kerr background using a continued-fraction method, adapted from studies of quasinormal modes. We demonstrate that the instability is most significant for the $l=1$, $m=1$ state, for Mμ0.5. For a fast rotating hole ($a=0.99$) we find a maximum growth rate of τ^-1≈1.5×10^-7(GM/c³)^-1, at Mμ≈0.42. The physical implications are discussed.
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Sam R. Dolan (2007) studied this question.
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