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The process of photon splitting in a strong
magnetic field is investigated both below and above the pair creation
threshold. Contrary to the statement by Baier et al., the allowed'' channel $\alw$ is shown not to be a comprehensive description of splitting in the strong field because the forbidden’’ channel is also essential. The
partial amplitudes and the splitting probabilities are calculated taking
account of the photon dispersion and large radiative corrections near the
resonance.

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