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The specific heat of UCd11 was measured in magnetic fields to 27T. Besides the antiferromagnetic transition, there is a second transition that can be clearly resolved in fields between 14 and 20T. This second transition (at Tm) extrapolates to a broad shoulder in C∕T in zero field. The two lines of transitions cross somewhere between 20 and 23T. Tm displays unusually weak dependence on the strength of the magnetic field. Our results argue for the intrinsic origin of this “hidden” transition.

Magnetic field study of the “hidden transition” in UCd11