# Universal mechanism of Ising superconductivity in twisted bilayer, trilayer and quadrilayer graphene

## TL;DR

This paper reveals a universal mechanism for superconductivity in twisted multilayer graphene, driven by valley symmetry breaking and Fermi line nesting, which explains the emergence and fading of superconductivity with doping.

## Contribution

It demonstrates that valley symmetry breaking and Fermi line nesting are fundamental to superconductivity across twisted bilayer, trilayer, and quadrilayer graphene, providing a unified theoretical framework.

## Key findings

- Superconductivity arises from valley symmetry breaking in moiré systems.
- Fermi line nesting induces a strong Kohn-Luttinger pairing instability.
- Superconductivity diminishes as the Fermi line becomes more isotropic at higher doping.

## Abstract

We show that the superconducivity in twisted graphene multilayers originates from a common feature, which is the strong valley symmetry breaking characteristic of these moir\'e systems at the magic angle. This leads to a breakdown of the rotational symmetry of the flat moir\'e bands down to $C_3$, and to ground states in which the time-reversal symmetry is broken for a given spin projection. However, this symmetry can be recovered upon exchange of spin-up and spin-down electrons, as we illustrate by means of a self-consistent microscopic Hartree-Fock resolution where the states for the two spin projections acquire opposite sign of the valley polarization. There is then a spin-valley locking by which the Fermi lines for the two spin projections are different and related by inversion symmetry. This effect represents a large renormalization of the bare spin-orbit coupling of the graphene multilayers, lending protection to the superconductivity against in-plane magnetic fields. In the twisted bilayer as well as in trilayer and quadrilayer graphene, the pairing glue is shown to be given by the nesting between parallel segments of the Fermi lines which arise from the breakdown of symmetry down to $C_3$. This leads to a strong Kohn-Luttinger pairing instability, which is relevant until the Fermi line recovers gradually a more isotropic shape towards the bottom of the second valence band, explaining why the superconductivity fades away beyond three-hole doping of the moir\'e unit cell.