Observation of an energy-symmetric flat-bottom U-shaped gap with zero residual DOS in (La,Pr)3Ni2O7 thin films, showing unconventional temperature evolution and magnetic field suppression consistent with a nodeless superconducting gap.
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4 Pith papers cite this work. Polarity classification is still indexing.
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UNVERDICTED 4representative citing papers
Single-crystal neutron scattering establishes stripe antiferromagnetic order with strong interlayer coupling and competing in-plane exchanges in La3Ni2O7, yielding fluctuating moments comparable to cuprates but with lower bandwidth.
Superconductivity in bilayer nickelates occurs in SDW-free oxygen-stoichiometric regions, with an interlayer five-spin polaron proposed as the ground state.
Superconductivity up to Tc=4 K emerges in UAs2 under pressure together with strange-metal resistivity and high upper critical field, vanishing at higher pressures with return to Fermi-liquid behavior.
citing papers explorer
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Observation of flat-bottom U-shaped energy gap in high-Tc nickelate (La,Pr)3Ni2O7 thin films
Observation of an energy-symmetric flat-bottom U-shaped gap with zero residual DOS in (La,Pr)3Ni2O7 thin films, showing unconventional temperature evolution and magnetic field suppression consistent with a nodeless superconducting gap.
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Nature of magnetism in bilayer nickelate La3Ni2O7 single crystals
Single-crystal neutron scattering establishes stripe antiferromagnetic order with strong interlayer coupling and competing in-plane exchanges in La3Ni2O7, yielding fluctuating moments comparable to cuprates but with lower bandwidth.
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Interlayer Five-Spin Polaron in Superconducting Bilayer Nickelates
Superconductivity in bilayer nickelates occurs in SDW-free oxygen-stoichiometric regions, with an interlayer five-spin polaron proposed as the ground state.
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Unconventional superconductivity emerging along with the strange-metal behavior in UAs2 under pressure
Superconductivity up to Tc=4 K emerges in UAs2 under pressure together with strange-metal resistivity and high upper critical field, vanishing at higher pressures with return to Fermi-liquid behavior.