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o as a free parameter but neglecting the finite width of the wires of the pickup loop (0.8 μm), the field expelled by the shielded leads, and the angle between the loop and the surface (∼20°), it is possible to describe the amplitude and shape of monopole (point-like) sources of magnetic flux to within 10%.
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note
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We thank P. W. Anderson, S. Chakravarty, S. Das Sarma, N. P. Ong, D. Scalapino, and D. van der Marel for useful discussions; D. Johnson for technical assistance in sample preparation; and M. Bhushan, M. Ketchen, and A. Ellis for assistance in the construction of the scanning SQUID microscope. Work at Argonne was supported by NSF grant DMR 91-20000 through the Science and Technology Center for Superconductivity, and by the U.S. Department of Energy under contract W-31-109-ENG-38. Work at Princeton was supported by NSF grant DMR 94-00362 through the Princeton Materials Institute, and by an R. H. Dicke Postdoctoral Fellowship.
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