Thomas R. Lemberger, John Draskovic
We consider the first appearance of vortices in a two-dimensional (2-D) superconducting film exposed to a non-uniform magnetic field, $\mathbf{B_a}$, produced by a nearby coil. The film has "infinite" radius, $R_f$, and thickness $t$ about equal to the coherence length, $\xi$. The coil is approximated as a point dipole. We find that the first vortex-bearing state to appear has both a vortex and an antivortex. The Gibbs free energy of this state is lower than the vortex-free state when the applied perpendicular field, $B_0$, at the origin exceeds the external critical field: $B_{c1}^0 = \frac{4\sqrt{2}\Lambda}{R}\frac{\Phi_0}{4\pi \Lambda^2}ln\left(\frac{\Lambda}{\xi}\right)$, where $\frac{\Phi_0}{4\pi\Lambda^2}ln\left(\frac{\Lambda}{\xi}\right) \equiv B_{c1}^{2D}$ is the intrinsic critical field in 2-D, $\Lambda \equiv 2\lambda^2/t$ the 2-D penetration depth introduced by Pearl, and $\lambda$ is the bulk penetration depth. The prefactor, $4\sqrt{2}\Lambda/R$, is calculated in the strong-screening regime, $\Lambda/R \ll 1$. $R$ is the radial distance at which the applied perpendicular field, $B_{a,z}(\rho)$, changes sign. In the lab, the onset of vortex effects generally occurs at a field much higher than $B_{c1}^0$, indicating that vortices are inhibited by the vortex-antivortex unbinding barrier, or by pinning.
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http://arxiv.org/abs/1302.0896
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