2014/12/31 by Michael Schütt, Rafael M. Fernandes · 11 citations
Materials Science · Physics and Astronomy · #Advanced Condensed Matter Physics #Anisotropy #Boltzmann constant #Charge (physics) #Condensed matter physics #Cuprate #Doping #Electrical resistivity and conductivity #Magnetic and transport properties of perovskites and related materials #Physics #Physics of Superconductivity and Magnetism #Quantum mechanics #Scattering #Spin (aerodynamics) #Superconductivity #cond-mat.str-el #cond-mat.supr-con
paper · pdf · doi:10.1103/physrevlett.115.027005
published in Physical Review Letters 115(2), 027005 (American Physical Society) · 5 pages + Supplementary Material
openalex publication_date 2015/07/09 · arxiv created 2015/09/03 · arxiv updated 2015/09/04 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
One of the prime manifestations of an anisotropic electronic state in underdoped cuprates is the in-plane resistivity anisotropy \mathrm\ensuremathΔ\ensuremathρ\ensuremath≡(\ensuremathρa\ensuremath-\ensuremathρb)/\ensuremathρb. Here we use a Boltzmann-equation approach to compute the contribution to \mathrm\ensuremathΔ\ensuremathρ arising from scattering by anisotropic charge and spin fluctuations, which have been recently observed experimentally. While the anisotropy in the charge fluctuations is manifested in the correlation length, the anisotropy in the spin fluctuations emerges only in the structure factor. As a result, we find that spin fluctuations favor \mathrm\ensuremathΔ\ensuremathρ>0, whereas charge fluctuations promote \mathrm\ensuremathΔ\ensuremathρ<0, which are both consistent with the doping dependence of \mathrm\ensuremathΔ\ensuremathρ observed in YBa2Cu3O7. We also discuss the role played by CuO chains in these materials, and propose transport experiments in strained HgBa2CuO4 and Nd2CuO4 to probe directly the different resistivity anisotropy regimes.