Flat band superconductivity in a system with a tunable quantum metric : the stub lattice

Over the past years, one witnesses a growing interest in flat band (FB) physics which has become a playground for exotic phenomena. In this study, we address the FB superconductivity in onedimensional stub chain. In contrast to the sawtooth chain or the creutz ladder, for a given strength of the attractive electron-electron interaction, the stub chain allows the tuning of the real space spreading of the FB eigenstates (quantum metric or QM). We study in detail the interplay between the interaction strength and the mean value of the QM \langle g \rangle on the pairings and on the superfluid weight D_s. Our calculations reveal several interesting and intriguing features. For instance, in the weak coupling regime, D_s with respect to \langle g \rangle exhibits two different types of behaviour. Despite the fact that the pairings differs drastically, D_s scales linearly with the QM only when its \langle g \rangle is large enough (small gap limit). On the other hand, when the QM is of small amplitude an unusual power law is found, more precisely D_s \propto \langle g \rangle^\nu where \nu \longrightarrow 2 in the limit of large single particle gap. In addition to the numerical calculations, we have provided several analytical results which shed light on the physics in both the weak and strong coupling regime. Finally, we have addressed the impact of the thermal fluctuations on the superfluid weight.Comment: 9 pages, 6 figures, published in PR

Constrain relations for superfluid weight and pairings in a chiral flat band superconductor

Abstract Within ten years, flat band (FB) superconductivity has gained a huge interest for its remarkable features and connection to quantum geometry. We investigate the superconductivity in a FB system whose orbitals are inequivalent and in which the gap and the quantum metric are tunable. 
The key feature of the present theoretical study is to show a unique and simple constrain relation that pairings obey. 
Furthermore, pairings and superfluid weight in partially filled FB are shown to be controlled by those of the half-filled lattice.
We argue that the geometry of the lattice or the complexity of the hopping terms have no impact on the features revealed in this work as far as the system is bipartite