Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
Rhombohedral trilayer graphene in the intervalley-coherent / superconducting regime analyzed with a low-energy Dirac-cone toy model and a microscopic band-structure-based model.
Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
Rhombohedral trilayer graphene in the intervalley-coherent / superconducting regime analyzed with a low-energy Dirac-cone toy model and a microscopic band-structure-based model.
Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
Rhombohedral trilayer graphene in the intervalley-coherent / superconducting regime analyzed with a low-energy Dirac-cone toy model and a microscopic band-structure-based model.
Each sample groups how it was prepared, characterized, and measured. Click a card to expand.
Rhombohedral trilayer graphene in the intervalley-coherent / superconducting regime analyzed with a low-energy Dirac-cone toy model and a microscopic band-structure-based model.
Analytical toy model of gapped Dirac cones with quasiparticle pairing near the IVC–flavor-symmetric boundary; numerical evaluation of superconducting transition temperature and upper critical field; microscopic model based on the 6-band Hamiltonian for rhombohedral trilayer graphene.
Settings
target stateintervalley coherent state
model componentsgapped Dirac cones, 6-band Hamiltonian
base temperature mK50
chemical potential meV-43.4
superconducting regimeSC₁
reference density cm^-2-1,850,000,000,000
carrier density window cm^-2-1930000000000, -1800000000000
Analytical toy model of gapped Dirac cones with quasiparticle pairing near the IVC–flavor-symmetric boundary; numerical evaluation of superconducting transition temperature and upper critical field; microscopic model based on the 6-band Hamiltonian for rhombohedral trilayer graphene.
Settings
target stateintervalley coherent state
model componentsgapped Dirac cones, 6-band Hamiltonian
base temperature mK50
chemical potential meV-43.4
superconducting regimeSC₁
reference density cm^-2-1,850,000,000,000
carrier density window cm^-2-1930000000000, -1800000000000
Analytical toy model of gapped Dirac cones with quasiparticle pairing near the IVC–flavor-symmetric boundary; numerical evaluation of superconducting transition temperature and upper critical field; microscopic model based on the 6-band Hamiltonian for rhombohedral trilayer graphene.
Settings
target stateintervalley coherent state
model componentsgapped Dirac cones, 6-band Hamiltonian
base temperature mK50
chemical potential meV-43.4
superconducting regimeSC₁
reference density cm^-2-1,850,000,000,000
carrier density window cm^-2-1930000000000, -1800000000000
Analytical toy model of gapped Dirac cones with quasiparticle pairing near the IVC–flavor-symmetric boundary; numerical evaluation of superconducting transition temperature and upper critical field; microscopic model based on the 6-band Hamiltonian for rhombohedral trilayer graphene.
Settings
target stateintervalley coherent state
model componentsgapped Dirac cones, 6-band Hamiltonian
base temperature mK50
chemical potential meV-43.4
superconducting regimeSC₁
reference density cm^-2-1,850,000,000,000
carrier density window cm^-2-1930000000000, -1800000000000
