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The magnetic moments of the low lying, negative parity, spin-3/2 baryons arecalculated within the light cone QCD sum rules method. The contributions comingfrom the positive parity, spin-3/2 baryons, as well as from the positive andnegative parity spin-1/2 baryons are eliminated by constructing combinations ofvarious invariant amplitudes corresponding to the coefficients of the differentLorentz structures.

Magnetic moments of $J^P = {3\over 2}^-$ baryons in QCD