A magnetic origin of cuprate superconductivity? A MaxEnt-μSR view

The fundamental physics of cuprate superconductivity is still much deliberated after three decades of research. In contrast to phononic or polaronic roots, some major theories promote a magnetic origin. In this perspective, we review cuprate magnetism, as probed by muon-spin-rotation (μSR) in RBa2Cu3O7−δ (RBCO), Bi2Sr2CaCu2O8+x (Bi2212) and Tl2Ba2Ca2Cu3O10+x (Tl2223). Site-search RBCO studies show that muons localize and probe in locations away from the superconducting CuO2 planes. Maximum entropy (MaxEnt, ME) analysis of transverse field μSR data of GdBa2Cu3O7−δ (GdBCO) indicates that the muon probes in an undisturbed insulating environment, allowing μSR to detect (weak) magnetic features in these cuprates. Concerning Varma’s predicted loop currents, MaxEnt has shown weak μSR signals for GdBCO in zero field above and below the critical temperature, Tc; these are near the predicted ∼ 100 Oe. Concerning Zhang’s predicted antiferromagnetism (AF) connected to the vortex cores, we have observed Lorentzian relaxation of cuprate vortex signals below half Tc, consistent with AF-broadening effects. For both Bi2212 and Tl2223, Lorentzians describe the μSR vortex signals much better below 0.4Tc than Gaussians, indicating that extra AF fields occur near and in the vortex cores. In sum, both our MaxEnt-μSR (ME-μSR) studies point toward magnetic roots of cuprate superconductivity.

[1]  R. Laughlin Fermi-liquid computation of the phase diagram of high-Tc cuprate superconductors with an orbital antiferromagnetic pseudogap. , 2014, Physical review letters.

[2]  M. Browne,et al.  Pseudogap and cuprate superconductivity: MaxEnt-μSR studies , 2013 .

[3]  Zahid Hussain,et al.  Phase competition in trisected superconducting dome , 2012, Proceedings of the National Academy of Sciences.

[4]  C. Varma High-temperature superconductivity: Mind the pseudogap , 2010, Nature.

[5]  M. Browne,et al.  Predicted Magnetic Fields of Loop Currents for Cuprate Superconductivity: A MaxEnt-μSR GdBCO Study , 2010 .

[6]  J. Roos,et al.  Lack of evidence for orbital-current effects in the high-temperature Y2Ba4Cu7O15-delta superconductor using 89Y nuclear magnetic resonance. , 2008, Physical review letters.

[7]  S. Wakimoto,et al.  Absence of broken time-reversal symmetry in the pseudogap state of the high temperature La(2-x)SrxCuO4 superconductor from muon-spin-relaxation measurements. , 2008, Physical review letters.

[8]  C. Varma,et al.  Screening of point charge impurities in highly anisotropic metals: application to mu+-spin relaxation in underdoped cuprate superconductors. , 2008, Physical Review Letters.

[9]  J. C. Lee,et al.  Magnetism in and near YBa2Cu3O7 vortex cores and its field dependence , 2007 .

[10]  D. Pines,et al.  The pseudogap: friend or foe of high T c ? , 2005, cond-mat/0507031.

[11]  L. Hughes,et al.  Plausiblity of Antiferromagnetism in and near RBCO Vortex Cores , 2003 .

[12]  W. H. Hardy,et al.  Evidence for static magnetism in the vortex cores of ortho-II YBa2Cu3O6.50. , 2001, Physical review letters.

[13]  N. Curro,et al.  Correlations between charge ordering and local magnetic fields in overdoped YBa 2 Cu 3 O 6 + x , 2001, cond-mat/0108479.

[14]  D. W. Cooke,et al.  d-Wave symmetry in Bi2212 and TI2223 vortex states: an ME-μSR study , 2000 .

[15]  Shou-Cheng Zhang,et al.  Superconducting Vortex with Antiferromagnetic Core , 1997, cond-mat/9704048.

[16]  Smith,et al.  Muon depolarization and magnetic-field penetration depth in superconducting GdBa2Cu3Ox. , 1988, Physical Review B (Condensed Matter).