Bipartite charge fluctuations in 3D metals encode Fermi surface geometry and quantum metric via a logarithmic term expressible as surface integrals of curvature and quantum metric tensors.
Title resolution pending
8 Pith papers cite this work. Polarity classification is still indexing.
8
Pith papers citing it
citation-role summary
background 2
citation-polarity summary
verdicts
UNVERDICTED 8roles
background 2polarities
background 2representative citing papers
Coulomb interactions turn a Berry-dipole semimetal into an anisotropic non-Fermi liquid with amplified topological Berry dipole under renormalization-group flow.
Surface fRG extension shows d-wave superconductivity from the 2D Hubbard model persists across most interlayer couplings but splits into two regimes separated by a narrow region of incommensurate spin-density-wave and spin-bond order at intermediate couplings.
The renormalized fermionic Casimir energy between parallel plates is modified only by the normal component of the axial background vector b_z, which combines with the timelike b_0 into a single effective spectral parameter in a closed logarithmic integral representation.
Spin-texture coupling to thin-film Dirac semimetals produces Weyl semimetals exhibiting anomalous Hall and chiral magnetic effects, plus Floquet-driven nodal spheres in momentum space.
Spatially varying light generates effective pseudo-magnetic fields in 3D Weyl semimetals via a high-frequency Floquet expansion that maps light profiles to an axial gauge potential A5(r).
Zn substitution stabilizes ferromagnetism in EuMn2Sb2 and induces Weyl nodes near the Fermi level through broken time-reversal and inversion symmetries.
A review summarizing theoretical and experimental progress on disorder-induced topological phases including TAIs, quasiperiodic extensions, non-Hermitian systems, and many-body realizations.
citing papers explorer
-
Fermi Surface Geometry from Charge Fluctuations in Three-Dimensional Metals
Bipartite charge fluctuations in 3D metals encode Fermi surface geometry and quantum metric via a logarithmic term expressible as surface integrals of curvature and quantum metric tensors.
-
Topological anisotropic non-Fermi liquid from a Berry-dipole semimetal
Coulomb interactions turn a Berry-dipole semimetal into an anisotropic non-Fermi liquid with amplified topological Berry dipole under renormalization-group flow.
-
Surface Functional Renormalization Group for Layered Quantum Materials
Surface fRG extension shows d-wave superconductivity from the 2D Hubbard model persists across most interlayer couplings but splits into two regimes separated by a narrow region of incommensurate spin-density-wave and spin-bond order at intermediate couplings.
-
Fermionic Casimir effect in an axial Lorentz-violating background
The renormalized fermionic Casimir energy between parallel plates is modified only by the normal component of the axial background vector b_z, which combines with the timelike b_0 into a single effective spectral parameter in a closed logarithmic integral representation.
-
Emergent Nodal Spheres and Weyl Fermions via Spin-Texture Coupled to Thin Film Orbital Dirac Semimetals
Spin-texture coupling to thin-film Dirac semimetals produces Weyl semimetals exhibiting anomalous Hall and chiral magnetic effects, plus Floquet-driven nodal spheres in momentum space.
-
Light-induced pseudo-magnetic fields in three-dimensional topological semimetals
Spatially varying light generates effective pseudo-magnetic fields in 3D Weyl semimetals via a high-frequency Floquet expansion that maps light profiles to an axial gauge potential A5(r).
-
Broken Symmetry-driven Weyl Semimetal Phase in Zn-Substituted EuMn$_2$Sb$_2$
Zn substitution stabilizes ferromagnetism in EuMn2Sb2 and induces Weyl nodes near the Fermi level through broken time-reversal and inversion symmetries.
-
Recent progress on disorder-induced topological phases
A review summarizing theoretical and experimental progress on disorder-induced topological phases including TAIs, quasiperiodic extensions, non-Hermitian systems, and many-body realizations.