A controlled expansion in s² for electrons with concentrated kinematics allows analytical calculations of spectral broadening, T-linear resistivity in bad metals, and spectral functions in Mott semimetals for Hubbard and Chern band models.
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4 Pith papers cite this work. Polarity classification is still indexing.
representative citing papers
In the topological heavy fermion model, the Mott semimetal phase hosts well-defined quasiparticles with dispersion and relaxation rate proportional to the interaction strength.
A new theoretical framework enables the quantum twisting microscope to perform momentum-resolved spectroscopy of superconductivity, extracting pairing magnitude and symmetry from tunneling channels in 2D materials.
DFT study of relaxed twisted bilayer graphene structures and bands for twist angles down to 0.987 degrees, with good agreement to continuum models except for a small angle offset.
citing papers explorer
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Controlled expansion for correlated electrons with concentrated kinematics
A controlled expansion in s² for electrons with concentrated kinematics allows analytical calculations of spectral broadening, T-linear resistivity in bad metals, and spectral functions in Mott semimetals for Hubbard and Chern band models.
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Lifetime and spectral function of topological heavy fermions
In the topological heavy fermion model, the Mott semimetal phase hosts well-defined quasiparticles with dispersion and relaxation rate proportional to the interaction strength.
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Momentum-resolved spectroscopy of superconductivity with the quantum twisting microscope
A new theoretical framework enables the quantum twisting microscope to perform momentum-resolved spectroscopy of superconductivity, extracting pairing magnitude and symmetry from tunneling channels in 2D materials.
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Twisted bilayer graphene from first-principles: structural and electronic properties
DFT study of relaxed twisted bilayer graphene structures and bands for twist angles down to 0.987 degrees, with good agreement to continuum models except for a small angle offset.