Interplay of superconductivity and spin density wave order in doped graphene
arXiv:1207.5802 · doi:10.1103/PhysRevB.86.115426
Abstract
We study the interplay between superconductivity and spin density wave order in graphene doped to 3/8 or 5/8 filling (a Van Hove doping). At this doping level, the system is known to exhibit weak coupling instabilities to both chiral d + id superconductivity and to a uniaxial spin density wave. Right at van Hove doping, the superconducting instability is strongest and emerges at the highest Tc, but slightly away from van-Hove doping a spin-density-wave likely emerges first. We investigate whether at some lower temperature superconductivity and spin-density-waves co-exist. We derive the Landau-Ginzburg functional describing interplay of the two order parameters. Our calculations show that superconductivity and spin density wave order do not co-exist and are separated by first-order transitions, either as a function of doping or as a function of T.
References in corpus (17)
- The electronic properties of graphene
- Paired states of fermions in two dimensions with breaking of parity and time-reversal symmetries, and the fractional quantum Hall effect
- Chiral superconductivity from repulsive interactions in doped graphene
- Superconducting states of pure and doped graphene
- Scalar spin chirality and quantum Hall effect on a triangular lattice
- Resonating valence bonds and mean-field d-wave superconductivity in graphite
- Functional renormalization group and variational Monte Carlo studies of the electronic instabilities in graphene near 1/4 doping
- Competing order and nature of the pairing state in the iron pnictides
- Kohn-Luttinger superconductivity in graphene
- Superconductivity and spin-density-waves in multi-band metals
- Electronic multicriticality in bilayer graphene
- Itinerant half-metal spin-density-wave state on the hexagonal lattice
- Spontaneous quantum Hall effect in quarter-doped Hubbard model on honeycomb lattice and its possible realization in quarter-doped graphene system
- Spin-density-wave instability in graphene doped near the van Hove singularity
- Pomeranchuk instability in doped graphene
- Coexistence between superconducting and spin density wave states in iron-based superconductors: Ginzburg-Landau analysis
- Prediction and description of a chiral pseudogap phase
Cited by in corpus (20)
- CsVSb: a topological kagome metal with a superconducting ground state
- Superconductivity in the kagome metal KVSb
- Electronic instabilities of kagome metals: saddle points and Landau theory
- Chiral d-wave superconductivity in doped graphene
- Superconductivity from weak repulsion in hexagonal lattice systems
- Chiral triplet superconductivity on the graphene lattice
- Chiral d-wave superconductivity on the honeycomb lattice close to the Mott state
- Instabilities of Weyl-loop semi-metals
- Loop currents and anomalous Hall effect from time-reversal symmetry-breaking superconductivity on the honeycomb lattice
- Possible singlet and triplet superconductivity on honeycomb lattice
- Defects in the (d+id)-wave superconducting state in heavily doped graphene
- On the coexistence of antiferromagnetism and d + i d superconducting correlations in the graphene bilayer
- The Kohn-Luttinger effect and anomalous pairing in new superconducting systems and graphene
- Particle-hole condensates of higher angular momentum in hexagonal systems
- Kekulé superconductivity and antiferromagnetism on the graphene lattice
- Superconductivity of strongly correlated electrons on the honeycomb lattice
- Anomalous superconductivity and superfluidity in repulsive fermion systems
- Fractal non-Fermi liquids from moiré-Hofstadter phonons
- Moiré surface states and enhanced superconductivity in topological insulators
- Mean-field analysis of a Hubbard interaction on Bernal Bilayer Graphene