A real-space dynamical embedding Green's function method enables first-principles calculations of superconducting proximity lengths and spectral functions in mesoscopic systems and heterostructures.
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A general construction using CFT null vectors and BPZ equations yields continuum Hamiltonians for which Moore-Read and k=3 Read-Rezayi Jack-polynomial states are exact zero modes.
Local twist operators and a purity-gap-based chiral marker provide practical real-space indicators of topology in finite-temperature mixed states of the SSH model.
Lattice models with engineered quantum geometry host Abelian and non-Abelian fractional Chern insulators, anomalous Hall crystals, and Halperin states, with the N=2 model realizable in twisted MoTe₂.
2DEG-S hybrids in quantized magnetic field host topologically protected edge states carrying even-integer quantized spin current robust to disorder.
A new protocol for layer-resolved transport measurements that extracts anyon statistics from charge distribution across layers in multi-component topological states.
A variational generalized Landau-level mapping shows the first moiré valence band supports Jain-sequence Abelian states while the Hartree-Fock-renormalized second band hosts a non-Abelian Moore-Read state at filling 5/2 for twist angle 2.45°.
CF exciton trial states accurately capture collective mode dispersions in spinful FQH states on the sphere at all wavelengths, while density-wave states miss high-energy parton modes in singlet cases at fillings like 2/5.
Sign changes of the new Krylov staggering parameter mark the boundary between edge-localized and bulk-dominated low-energy regimes in the Kitaev chain.
citing papers explorer
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First-principles real-space embedding theory of the superconducting proximity effect
A real-space dynamical embedding Green's function method enables first-principles calculations of superconducting proximity lengths and spectral functions in mesoscopic systems and heterostructures.
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Parent Hamiltonian Construction of Generalized Calogero-Sutherland Models
A general construction using CFT null vectors and BPZ equations yields continuum Hamiltonians for which Moore-Read and k=3 Read-Rezayi Jack-polynomial states are exact zero modes.
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Characterizing topology at nonzero temperature: Topological invariants and indicators in the extended SSH model
Local twist operators and a purity-gap-based chiral marker provide practical real-space indicators of topology in finite-temperature mixed states of the SSH model.
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Quantum-Geometric Design of Lattice Generalized Landau Levels
Lattice models with engineered quantum geometry host Abelian and non-Abelian fractional Chern insulators, anomalous Hall crystals, and Halperin states, with the N=2 model realizable in twisted MoTe₂.
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Emergent spin quantum Hall edge states at the boundary of two-dimensional electron gas proximitized by an $s$-wave superconductor
2DEG-S hybrids in quantized magnetic field host topologically protected edge states carrying even-integer quantized spin current robust to disorder.
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Probing bilayer topological order with layer-resolved transport
A new protocol for layer-resolved transport measurements that extracts anyon statistics from charge distribution across layers in multi-component topological states.
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Abelian and non-Abelian fractionalized states in twisted MoTe$_2$: A generalized Landau-level theory
A variational generalized Landau-level mapping shows the first moiré valence band supports Jain-sequence Abelian states while the Hartree-Fock-renormalized second band hosts a non-Abelian Moore-Read state at filling 5/2 for twist angle 2.45°.
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Dispersion of collective modes in spinful fractional quantum Hall states on the sphere
CF exciton trial states accurately capture collective mode dispersions in spinful FQH states on the sphere at all wavelengths, while density-wave states miss high-energy parton modes in singlet cases at fillings like 2/5.
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Long-Range Pairing in the Kitaev Model: Krylov Subspace Signatures
Sign changes of the new Krylov staggering parameter mark the boundary between edge-localized and bulk-dominated low-energy regimes in the Kitaev chain.