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.
Chalopin , author P
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Experimental demonstration of collisional spin-exchange and pair-tunneling gates on fermionic atoms achieving up to 99.75(6)% fidelity and Bell-state lifetimes over 10 seconds.
The fractionalized Fermi liquid state obtained by doping quantum spin liquids resolves key experimental difficulties in cuprate pseudogap metals and d-wave superconductors.
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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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High-fidelity collisional quantum gates with fermionic atoms
Experimental demonstration of collisional spin-exchange and pair-tunneling gates on fermionic atoms achieving up to 99.75(6)% fidelity and Bell-state lifetimes over 10 seconds.
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Lectures on insulating and conducting quantum spin liquids
The fractionalized Fermi liquid state obtained by doping quantum spin liquids resolves key experimental difficulties in cuprate pseudogap metals and d-wave superconductors.