A universal magnetic energy scale J* emerges at finite doping in the Fermi-Hubbard model, controlling magnetic correlations, bimagnon spectra, pseudogap onset, and the transition to incommensurate spin-density waves.
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Uniaxial pressure applied to α-SrCr₂O₄ shifts two-magnon Raman excitations in a manner consistent with decreased or increased magnetic anisotropy under tension or compression.
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Universal magnetic energy scale in the doped Fermi-Hubbard model
A universal magnetic energy scale J* emerges at finite doping in the Fermi-Hubbard model, controlling magnetic correlations, bimagnon spectra, pseudogap onset, and the transition to incommensurate spin-density waves.
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Tuning J$_1$-J$_2$ in Quasi-2D Triangular Lattice Antiferromagnet $\alpha$-SrCr$_2$O$_4$ via Uniaxial Pressure
Uniaxial pressure applied to α-SrCr₂O₄ shifts two-magnon Raman excitations in a manner consistent with decreased or increased magnetic anisotropy under tension or compression.