Isolated bands with quantum metric exhibit a disorder-induced localization length plateau at approximately twice the quantum metric length, protected until disorder exceeds the band gap.
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Collective fluctuations generate dynamical Berry curvature via non-commutative transverse quantum fluctuations and non-local-time interactions, distinguishable from bare band geometry in antisymmetric inelastic scattering channels.
Nonlinear spin conductivity in Floquet non-Hermitian d-wave altermagnets separates into quantum-metric, Berry-curvature and dipole terms and is dominated by the bare quantum metric, with polarization reversing both longitudinal and transverse currents.
citing papers explorer
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Quantum Metric Localization and Quantum Metric Protection
Isolated bands with quantum metric exhibit a disorder-induced localization length plateau at approximately twice the quantum metric length, protected until disorder exceeds the band gap.
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Geometric curvature driven by many-body collective fluctuations
Collective fluctuations generate dynamical Berry curvature via non-commutative transverse quantum fluctuations and non-local-time interactions, distinguishable from bare band geometry in antisymmetric inelastic scattering channels.
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Quantum Geometry-Driven Nonlinear Spin Currents in Floquet Non-Hermitian Altermagnets
Nonlinear spin conductivity in Floquet non-Hermitian d-wave altermagnets separates into quantum-metric, Berry-curvature and dipole terms and is dominated by the bare quantum metric, with polarization reversing both longitudinal and transverse currents.