A human-in-the-loop multi-stage LLM workflow with an intermediate technical specification externalizing index conventions and contraction orders enables reliable DMRG code generation that reproduces known entanglement scaling and SPT order in spin chains, succeeding in all tested cases.
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Perturbations to the chiral Z_p toric code induce Hall-on-Toric descendant states featuring fractional Z_p charges and increased topological degeneracy, identified via iDMRG analysis of entanglement and generalized Hall conductance.
Electric field enhances ring exchange relative to Heisenberg interactions, shifting the CSL phase boundary to smaller t/U in the ring exchange model on the triangular lattice.
DMRG calculations on the two-leg Lieb ladder Hubbard model identify a ferrimagnetic insulator at half filling and a narrow superconducting Luther-Emery phase near filling 2/3.
citing papers explorer
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From Paper to Program: Accelerating Quantum Many-Body Algorithm Development via a Multi-Stage LLM-Assisted Workflow
A human-in-the-loop multi-stage LLM workflow with an intermediate technical specification externalizing index conventions and contraction orders enables reliable DMRG code generation that reproduces known entanglement scaling and SPT order in spin chains, succeeding in all tested cases.
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Hall-on-Toric: Descendant Laughlin state in the chiral $\mathbb{Z}_p$ toric code
Perturbations to the chiral Z_p toric code induce Hall-on-Toric descendant states featuring fractional Z_p charges and increased topological degeneracy, identified via iDMRG analysis of entanglement and generalized Hall conductance.
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Electric field control of a quantum spin liquid in weak Mott insulators
Electric field enhances ring exchange relative to Heisenberg interactions, shifting the CSL phase boundary to smaller t/U in the ring exchange model on the triangular lattice.
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From Ferrimagnetic Insulator to superconducting Luther-Emery Liquid: A DMRG Study of the Two-Leg Lieb Lattice
DMRG calculations on the two-leg Lieb ladder Hubbard model identify a ferrimagnetic insulator at half filling and a narrow superconducting Luther-Emery phase near filling 2/3.