Higher-order correlator families are recast as operator-space geometries that, when conditioned on a chosen subspace, reveal irreducible structures distinguishing free, integrable, chaotic, localized, and Floquet dynamics.
Sachdev, Quantum Phase Transitions, 2nd ed
2 Pith papers cite this work. Polarity classification is still indexing.
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Umklapp scattering near the zone boundary adds an Ω^{1/2} or Ω^{2/3} contribution to the particle-hole bubble in 2D Ising-nematic criticality, potentially shifting the onset of linear-in-T resistivity from Δ_q^3 to Δ_q^4 in one hyper-specific temperature regime.
citing papers explorer
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Irreducible Geometry of Higher-Order Correlator Families
Higher-order correlator families are recast as operator-space geometries that, when conditioned on a chosen subspace, reveal irreducible structures distinguishing free, integrable, chaotic, localized, and Floquet dynamics.
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Umklapp correction to Landau damping and conditions for non-trivial modifications to quantum critical transport
Umklapp scattering near the zone boundary adds an Ω^{1/2} or Ω^{2/3} contribution to the particle-hole bubble in 2D Ising-nematic criticality, potentially shifting the onset of linear-in-T resistivity from Δ_q^3 to Δ_q^4 in one hyper-specific temperature regime.