Finite-momentum pairing and superlattice superconductivity in valley-imbalanced rhombohedral graphene

Maine Christos; Pietro M. Bonetti; Mathias S. Scheurer

doi:10.1038/s41467-022-34832-2

Paper details

Research paper

TheoreticalComputational Multiscale

Finite-momentum pairing and superlattice superconductivity in valley-imbalanced rhombohedral graphene

Maine Christos, Pietro M. Bonetti, Mathias S. Scheurer

2025·10.1038/s41467-022-34832-2·arXiv:2503.15471

Samples

Each sample groups how it was prepared, characterized, and measured. Click a card to expand.

Continuum-model representation of valley-imbalanced rhombohedral tetralayer graphene in the active band, used to analyze pairing instabilities, Chern number, and finite-momentum superconducting states.

1 property

SimulatedCStudied Material

Materials

rhombohedral tetralayer graphene

Studied Material

Also known as

tetralayer rhombohedral graphenerhombohedral stacked tetralayer graphenegraphene

Variables

stacking= rhombohedral

layer_count

Why these are connected

Related documents with shared materials, methods, properties, or citations.

Finite-momentum pairing and superlattice superconductivity in valley-imbalanced rhombohedral graphene | Matter42 Literature

Finite-momentum pairing and superlattice superconductivity in valley-imbalanced rhombohedral graphene

Samples

Continuum-model representation of valley-imbalanced rhombohedral tetralayer graphene in the active band, used to analyze pairing instabilities, Chern number, and finite-momentum superconducting states.

Materials

Why these are connected

Finite-momentum pairing and superlattice superconductivity in valley-imbalanced rhombohedral graphene

Samples

Continuum-model representation of valley-imbalanced rhombohedral tetralayer graphene in the active band, used to analyze pairing instabilities, Chern number, and finite-momentum superconducting states.

Materials

Why these are connected

Finite-momentum pairing and superlattice superconductivity in valley-imbalanced rhombohedral graphene

Samples

Continuum-model representation of valley-imbalanced rhombohedral tetralayer graphene in the active band, used to analyze pairing instabilities, Chern number, and finite-momentum superconducting states.

Materials

Why these are connected

Finite-momentum pairing and superlattice superconductivity in valley-imbalanced rhombohedral graphene

Samples

Continuum-model representation of valley-imbalanced rhombohedral tetralayer graphene in the active band, used to analyze pairing instabilities, Chern number, and finite-momentum superconducting states.

Materials

Why these are connected

Finite-momentum pairing and superlattice superconductivity in valley-imbalanced rhombohedral graphene

Samples

Continuum-model representation of valley-imbalanced rhombohedral tetralayer graphene in the active band, used to analyze pairing instabilities, Chern number, and finite-momentum superconducting states.

Materials

Why these are connected

Finite-momentum pairing and superlattice superconductivity in valley-imbalanced rhombohedral graphene

Samples

Continuum-model representation of valley-imbalanced rhombohedral tetralayer graphene in the active band, used to analyze pairing instabilities, Chern number, and finite-momentum superconducting states.

Materials

Why these are connected

Finite-momentum pairing and superlattice superconductivity in valley-imbalanced rhombohedral graphene

Samples

Continuum-model representation of valley-imbalanced rhombohedral tetralayer graphene in the active band, used to analyze pairing instabilities, Chern number, and finite-momentum superconducting states.

Materials

Why these are connected

Finite-momentum pairing and superlattice superconductivity in valley-imbalanced rhombohedral graphene

Samples

Continuum-model representation of valley-imbalanced rhombohedral tetralayer graphene in the active band, used to analyze pairing instabilities, Chern number, and finite-momentum superconducting states.

Materials

Why these are connected

Properties

Simulations

Properties

Simulations

Properties

Simulations

Properties

Simulations