Effect of pressure on the Cu and Pr magnetism in Nd(1-x)Pr(x)Ba2Cu3O7 investigated by muon spin rotation
arXiv:1211.3584 · doi:10.1103/PhysRevB.87.054401
Abstract
The effect of pressure on the copper and praseodymium magnetic order in the system Nd(1-x)O7 with x=0.3, 0.5, 0.7, and 1 was investigated by means of the muon spin rotation (muSR) technique. It was found that the effect of pressure on the Neel temperatures of both copper and praseodymium is positive for the whole range of Pr concentrations (0.3<x<1) studied. These findings are in contrast with a number of previous reports and clarify some of the puzzles related to the effect of pressure on superconductivity and magnetism in the praseodymium-substituted R}(1-x)$Pr(x)Ba2Cu3O7 systems, where R is a rare earth element.
arXiv comment14 pages, 11 figures
References in corpus (6)
- Spin-polarized muons in condensed matter physics
- Oxygen isotope effect on superconductivity and magnetism in Y_1-xPr_xBa_2Cu_3O_7-δ
- Muon spin rotation investigation of the pressure effect on the magnetic penetration depth in YBa2Cu3Ox
- Where are holes in Y_{1-x}Pr_xBa2Cu3O7 ?
- On the possibility of superconductivity in PrBa2Cu3O7
- The phase transition in the localized ferromagnet EuO probed by muSR
Cited by in corpus (6)
- Direct evidence for the emergence of a pressure induced nodal superconducting gap in the iron-based superconductor Ba_0.65Rb_0.35Fe_2As_2
- Tuning the static spin-stripe phase and superconductivity in La_(2-x)Ba_xCuO_4 (x = 1/8) by hydrostatic pressure
- Cooperative coupling of static magnetism and bulk superconductivity in the stripe phase of La_2-xBa_xCuO_4: Pressure- and doping-dependent studies
- Probing the pairing symmetry in the over-doped Fe-based superconductor Ba_0.35Rb_0.65Fe_2As_2 as a function of hydrostatic pressure
- Probing the quantum phase transition in Mott insulator BaCoS_2 tuned by pressure and Ni-substitution
- Pressure tuning of structure, superconductivity and novel magnetic order in the Ce-underdoped electron-doped cuprate T'-Pr_1.3-xLa_0.7Ce_xCuO_4 (x = 0.1)