London screening
= London screening
{c}
{title2=$\nabla^2\mathbf B=\mathbf B/\lambda^2$}
Combining the static <London equations> with the <magnetostatic Ampère law> and $\nabla\cdot\mathbf B=0$ gives the displayed bulk equation for a uniform superconducting carrier density. A planar boundary gives exponentially decaying field on the <London penetration depth> scale; boundary geometry and vortices require their corresponding field solutions.