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Resistance of disordered superconducting AuIn cylindrical films was measured as a function of applied magnetic field. In the high-temperature part of the superconducting transition regime, the resistance oscillated with a period of in the unit of the enclosed magnetic flux. However, at lower temperatures, the resistance peaks split. We argue that this splitting is due to the emergence of an oscillation with a period of , half of the flux quantum for paired electrons. The possible physical origin of the resistance oscillation is discussed in the context of new minima in the free energy of a disordered superconducting cylinder.

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