2011/01/14 by M. V. Kartsovnik, M V Kartsovnik, T. Helm +23 · 1 citation
Physics and Astronomy · #Cuprate #Cyclotron #Fermi surface #Magnetic field #Magnetoresistance #Physics of Superconductivity and Magnetism #Quantum oscillations #Rare-earth and actinide compounds #Superconductivity #Superconductivity in MgB2 and Alloys #Superlattice #cond-mat.mtrl-sci #cond-mat.supr-con
paper · pdf · doi:10.1088/1367-2630/13/1/015001
published as New J. Phys. 13 015001 (2011) · 23 pages, 8 figures
openalex publication_date 2011/01/14 · arxiv created 2011/04/06 · arxiv updated 2015/03/18 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/06
We report on the study of the Fermi surface of the electron-doped cuprate superconductor Nd 2− x Ce x CuO 4 by measuring the interlayer magnetoresistance as a function of the strength and orientation of the applied magnetic field. We performed experiments in both steady and pulsed magnetic fields on high-quality single crystals with Ce concentrations of x =0.13–0.17. In the overdoped regime of x >0.15, we found both semiclassical angle-dependent magnetoresistance oscillations (AMROs) and Shubnikov–de Haas (SdH) oscillations. The combined AMROs and SdH data clearly show that the appearance of fast SdH oscillations in strongly overdoped samples is caused by magnetic breakdown. This observation provides clear evidence for a reconstructed multiply connected Fermi surface up to the very end of the overdoped regime at x ≃0.17. The strength of the superlattice potential responsible for the reconstructed Fermi surface is found to decrease with increasing doping level and likely vanishes at the same carrier concentration as superconductivity, suggesting a close relation between translational symmetry breaking and superconducting pairing. A detailed analysis of the high-resolution SdH data allowed us to determine the effective cyclotron mass and Dingle temperature, as well as to estimate the magnetic breakdown field in the overdoped regime.