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Non-quantized penetration of magnetic field in the vortex state of superconductors


As first pointed out by Bardeen and Ginzburg in the early sixties1,2, the amount of magnetic flux carried by vortices in superconducting materials depends on their distance from the sample edge, and can be smaller than one flux quantum, φ0 = h/2e (where h is Planck's constant and e is the electronic charge). In bulk superconductors, this reduction of flux becomes negligible at sub-micrometre distances from the edge, but in thin films the effect may survive much farther into the material3,4. But the effect has not been observed experimentally, and it is often assumed that magnetic field enters type II superconductors in units of φ0. Here we measure the amount of flux introduced by individual vortices in a superconducting film, finding that the flux always differs substantially from φ0. We have observed vortices that carry as little as 0.001φ0, as well as ‘negative vortices’, whose penetration leads to the expulsion of magnetic field. We distinguish two phenomena responsible for non-quantized flux penetration: the finite-size effect1,2,3,4 and a nonlinear screening of the magnetic field due to the presence of a surface barrier. The latter effect has not been considered previously, but is likely to cause non-quantized penetration in most cases.

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Figure 1: Penetration of perpendicular magnetic field in a thin superconducting film.
Figure 2: Penetration and expulsion of the first vortex in superconductors with various edge roughnesses.
Figure 3: Magnetic response of mesoscopic superconductors found theoretically.
Figure 4: The amount of magnetic flux associated with a vortex in the centre of a thin superconducting disk in equilibrium.


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We thank V. Kogan for discussions, and FOM, INTAS and NATO for financial support.

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Correspondence to A. K. Geim.

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Geim, A., Dubonos, S., Grigorieva, I. et al. Non-quantized penetration of magnetic field in the vortex state of superconductors . Nature 407, 55–57 (2000).

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