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We calculate the spin-dependent polarizability of the nucleon in the Skyrme model. The result is compared with that of a heavy baryon chiral perturbation theory(HBChPT), and is shown to be the same as that of HBChPT up to the -pole terms in the narrow width limit of the state and with the experimental physical constants. The effect of the channel is rather small and is numerically quite similar to that of the loop in the HBChPT. The electric and magnetic polarizabilities are recalculated using the transverse photon and a consistent inclusion of the width.

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