DMRG calculations provide evidence that Kondo-Heisenberg chains realize an interior-gap PDW superconducting state whose momentum distribution shows a characteristic hump or dip structure generated dynamically by interactions.
Title resolution pending
5 Pith papers cite this work. Polarity classification is still indexing.
5
Pith papers citing it
representative citing papers
A dipole-conserving spin chain with Ising interactions stabilizes antiferromagnetic dipole order at the level of spin pairs and undergoes transitions to conventional antiferromagnetic or ferromagnetic order depending on interaction sign and strength.
In the 1D Fermi-Hubbard model with opposing spin-dependent linear potentials, the ground state shows three regimes with a staircase-like reduction in bound pairs as the gradient increases, enabling integer-level control of pairing.
In a dimerized staggered Hubbard ring at half filling, the many-body Wilson loop satisfies the exact identity W(-δ) = W(δ)* even in regimes where the Berry phase is unquantized and varies continuously.
A driven dipole-conserving Bose-Hubbard model realizes controllable resonant splitting and motion of dipoles and fractons via engineered time-dependent tensor electric fields.
citing papers explorer
-
Evidence for interior-gap pair-density-wave state in Kondo-Heisenberg chains
DMRG calculations provide evidence that Kondo-Heisenberg chains realize an interior-gap PDW superconducting state whose momentum distribution shows a characteristic hump or dip structure generated dynamically by interactions.
-
Fractonic Constraints and Magnetic Order in a Dipole-Conserving Spin Chain
A dipole-conserving spin chain with Ising interactions stabilizes antiferromagnetic dipole order at the level of spin pairs and undergoes transitions to conventional antiferromagnetic or ferromagnetic order depending on interaction sign and strength.
-
Ground state of the Hubbard model with spin-dependent linear potential
In the 1D Fermi-Hubbard model with opposing spin-dependent linear potentials, the ground state shows three regimes with a staircase-like reduction in bound pairs as the gradient increases, enabling integer-level control of pairing.
-
An Exact Conjugation Identity for the Many-Body Wilson-Loop Beyond Quantization
In a dimerized staggered Hubbard ring at half filling, the many-body Wilson loop satisfies the exact identity W(-δ) = W(δ)* even in regimes where the Berry phase is unquantized and varies continuously.
-
Resonant dynamics of dipole-conserving Bose-Hubbard model with time-dependent tensor electric fields
A driven dipole-conserving Bose-Hubbard model realizes controllable resonant splitting and motion of dipoles and fractons via engineered time-dependent tensor electric fields.