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First non-trivial chiral corrections to the magnetic moments of triplet (T) and sextet () heavy baryons are presented using Heavy Hadron Chiral Perturbation Theory. The contributions are calculated up to order ${\cal O}(1/(m_Q \Lambda_\chi^2)){\cal O}(1/\Lambda_\chi^2)S^{(*)}$-baryons. The renormalization of the chiral loops is discussed and relations among the magnetic moments of different hadrons are provided.

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