2008/02/09 by C. Stock, Christian Stock, W. J. L. Buyers +8 · 1 citation
Materials Science · Physics and Astronomy · #Advanced Condensed Matter Physics #Magnetic and transport properties of perovskites and related materials #Physics of Superconductivity and Magnetism #cond-mat.supr-con
paper · pdf · doi:10.1103/physrevb.77.104513
22 pages, 19 figures, accepted for publication in Phys. Rev. B
arxiv created 2008/02/09 · openalex publication_date 2008/03/14 · arxiv updated 2009/12/01 · openalex created_date 2016/06/24 · openalex updated_date 2026/07/28
From neutron inelastic and elastic scattering we have determined the magnetic structure and fluctuations in the YBa2Cu3O6.35 (YBCO) superconductor (Tc=18\phantom\rule0.3em0exK) near the boundary of the superconducting phase. The long-range ordered collinear spins of the insulating antiferromagnet are replaced by a commensurate central mode arising from slow, isotropically polarized, short-range spin correlations extending over four planar unit cells. The inelastic spectrum up to 30\phantom\rule0.3em0exmeV is also broad in wave vector and commensurate. In contrast to the resonance peak of higher-Tc superconductors, the spins exhibit a single overdamped spectrum whose rate of relaxation \ensuremathΓ decreases on cooling and saturates at 2\ensuremathΓ=5\ifmmode±\else\textpm\fi1\phantom\rule0.3em0exmeV below \ensuremath∼50\phantom\rule0.3em0exK. As the relaxation rate saturates, the quasistatic spin correlations grow and become resolution limited in energy. The spin susceptibility above \ensuremath∼50\phantom\rule0.3em0exK follows the same \ensuremathω∕T scaling relation found for the monolayer La_2\ensuremath-xSrxCuO4 system, indicating that the dominant energy scale is set by the temperature. Below 50\phantom\rule0.3em0exK the scale length is geometric and not linked by velocity to dynamic widths. Despite the large differences from an antiferromagnet, we show that integrated intensity conserves the total moment sum rule, and that on cooling the spectral weight transfers from the inelastic spin relaxation to the elastic central peak. There is no observable suppression of the spin fluctuations or central mode upon the onset of superconductivity. The spins respond not to coherent charge pairs but to hole doping, allowing coexistence of glassy short-range spin order with superconductivity. Since the physics of the weakly superconducting system YBCO6.35 must connect continuously with that in more strongly superconducting YBCO6.5, we find that neither incommensurate stripe-like spin modulations nor a well-defined neutron spin resonance are essential for the onset with doping of pairing in a high-temperature cuprate superconductor.