The Ginzburg-Landau theory of flat-band superconductors with quantum metric

Recent experimental study unveiled highly unconventional phenomena in the superconducting twisted bilayer graphene (TBG) with ultra-flat bands, which cannot be described by the conventional BCS theory. For example, given the small Fermi velocity of the flat bands, the superconducting coherence length predicted by BCS theory is more than 20 times shorter than the measured values. A new theory is needed to understand many of the unconventional properties of flat-band superconductors. We establish a Ginzburg-Landau (GL) theory from a microscopic flat band Hamiltonian. The GL theory shows how the properties of the physical quantities such as the critical temperature, the superconducting coherence length, the upper critical field, and the superfluid density are governed by the quantum metric of the Bloch states. One key conclusion is that the superconducting coherence length is not determined by the Fermi velocity but by the size of the optimally localized Wannier functions which is limited by quantum metric. For a dispersive band with finite quantum metric,

the coherence length consists of both the quantum metric and conventional parts. We find that even the conventional parts are different between narrow-band systems and high-dispersive systems. Applying the theory to TBG, we calculated the superconducting coherence length and the upper critical fields.

The results match the experimental ones well without fine-tuning the parameters.