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note
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The reason why the range of φ for Fig. 13 is wider than for Fig. 12 is simply due to the difference in the magnetic decoration. First, the ferromagnetic material for sample B was nickel in contrast to cobalt for sample A. Secondly, the distance between the ferromagnet array and the superconducting network was about five times larger for sample B than sample A. These two factors made the value of φ required for the same amplitude of magnetic field modulation much larger for sample B than for sample A.
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