Negative electrohydrostatic pressure between superconducting bodies

Despite being largely limited to bulk phenomena, well-known theoretical models of superconductivity like the Bardeen-Cooper-Schrieffer and Ginzburg-Landau theories have played a key role in the development of superconducting quantum devices. In this letter, we present a hydrodynamic non-relativistic scalar electrodynamic theory capable of describing systems comprising superconducting materials of arbitrary shape and apply it to predict the existence of a negative (attractive) pressure between planar superconducting bodies. For conventional superconductors with London penetration depth $\lambda_\text{L} \approx 100 \text{ nm}$, the pressure reaches tens of $\text{N/mm}^2$ at angstrom separations.