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5 Pith papers cite this work. Polarity classification is still indexing.

5 Pith papers citing it

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2026 1 2025 4

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UNVERDICTED 5

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Universal Relations in Long-range Quantum Spin Chains

cond-mat.quant-gas · 2025-10-27 · unverdicted · novelty 7.0

Universal relations connect asymptotic equal-time spin correlations, dynamical structure factor, and contact density in long-range quantum spin chains via effective field theory and operator product expansion, with numerical verification.

Efimov Effect in Long-range Quantum Spin Chains

cond-mat.quant-gas · 2025-02-28 · unverdicted · novelty 7.0

Long-range interactions in quantum spin chains enable the Efimov effect for magnons by inducing continuous scale invariance in two-body states that becomes discrete in the three-body problem.

Qubit discretizations of d=3 conformal field theories

cond-mat.str-el · 2026-03-08 · unverdicted · novelty 6.0

A protocol extracts scaling dimensions of d=3 CFTs from the spectrum of qubit Hamiltonians on polyhedral lattices, achieving few-percent accuracy on the 3D Ising model with 20 qubits.

Trading athermality for nonstabiliserness

quant-ph · 2025-11-17 · unverdicted · novelty 6.0

Thermal operations can generate nonstabiliser states from stabilizer states, with an analytic characterization for qubits and a general trade-off between attainable nonstabiliserness and initial free energy.

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Showing 2 of 2 citing papers after filters.

  • Universal Relations in Long-range Quantum Spin Chains cond-mat.quant-gas · 2025-10-27 · unverdicted · none · ref 55

    Universal relations connect asymptotic equal-time spin correlations, dynamical structure factor, and contact density in long-range quantum spin chains via effective field theory and operator product expansion, with numerical verification.

  • Efimov Effect in Long-range Quantum Spin Chains cond-mat.quant-gas · 2025-02-28 · unverdicted · none · ref 39

    Long-range interactions in quantum spin chains enable the Efimov effect for magnons by inducing continuous scale invariance in two-body states that becomes discrete in the three-body problem.