NP-FRG computation shows the quantum RFIM has activated dynamics ln τ ~ ξ^Ψ at T=0, with Ψ set by classical RFIM static exponents and bare kernel exponent σ, crossing over to thermal activation at finite T.
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Neutron scattering reveals dynamical scaling of critical spin fluctuations across the LSCO superconducting dome, consistent with a disordered spin density wave quantum phase transition explaining strange metal behavior.
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Activated dynamics in the quantum random field Ising model
NP-FRG computation shows the quantum RFIM has activated dynamics ln τ ~ ξ^Ψ at T=0, with Ψ set by classical RFIM static exponents and bare kernel exponent σ, crossing over to thermal activation at finite T.
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Critical spin fluctuations across the superconducting dome in La$_{2-x}$Sr$_{x}$CuO$_4$
Neutron scattering reveals dynamical scaling of critical spin fluctuations across the LSCO superconducting dome, consistent with a disordered spin density wave quantum phase transition explaining strange metal behavior.