NMR shift disentanglement in cuprates reveals A and B spin components whose coupling defines the pseudogap temperature and whose balance sets optimal superconducting Tc.
As expected, the high-temperature B-spin draws the superconducting dome when plotted againstT c, as Fig
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Pseudogap and Condensation in Cuprate Superconductors from NMR Shifts
NMR shift disentanglement in cuprates reveals A and B spin components whose coupling defines the pseudogap temperature and whose balance sets optimal superconducting Tc.