NMR study of electronic correlations in Mn-doped Ba(Fe1-xCox)2As2 and BaFe(As1-xPx)2
arXiv:1310.4969 · doi:10.1103/PhysRevB.89.035114
Abstract
We probe the real space electronic response to a local magnetic impurity in isovalent and heterovalent doped BaFe2As2 (122) using Nuclear Magnetic Resonance (NMR). The local moments carried by Mn impurities doped into Ba(Fe1-xCox)2As2(Co-122) and BaFe(As1-xPx)2(P-122) at optimal doping induce a spin polarization in the vicinity of the impurity. The amplitude, shape and extension of this polarisation is given by the real part of the susceptibility chi'(r) of FeAs layers, and is consequently related to the nature and strength of the electronic correlations present in the system. We study this polarisation using 75As NMR in Co-122 and both 75As and 31P NMR in P-122. The NMR spectra of Mn-doped materials is made of two essential features. First is a satellite line associated with nuclei located as nearest neighbor of Mn impurities. The analysis of the temperature dependence of the shift of this satellite line shows that Mn local moments behave as isolated Curie moments. The second feature is a temperature dependent broadening of the central line. We show that the broadening of the central line follows the susceptibility of Mn local moments, as expected from typical RKKY-like interactions. This demonstrates that the susceptibility chi'(r) of FeAs layers does not make significant contribution to the temperature dependent broadening of the central line. chi'(r) is consequently only weakly temperature dependent in optimally doped Co-122 and P-122. This behaviour is in contrast with that of strongly correlated materials such as underdoped cuprate high-Tc superconductors where the central line broadens faster than the impurity susceptibility grows, because of the development of strong magnetic correlations when T is lowered. Moreover, the FeAs layer susceptibility is found quantitatively similar in both heterovalent doped and isolvalent doped BaFe2As2.
References in corpus (8)
- Superconductivity at 38 K in the iron arsenide (Ba1-xKx)Fe2As2
- High-temperature superconductivity in iron-based materials
- Superconductivity at 22 K in Co-doped BaFe2As2 Crystals
- Superconductivity up to 29 K in SrFe2As2 and BaFe2As2 at high pressures
- Superconductivity up to 30 K in the vicinity of quantum critical point in BaFe(AsP)
- Fermi surface of superconducting LaFePO determined by quantum oscillations
- Thermodynamic phase diagram and phase competition in BaFe2(As1-xPx)2 studied by thermal expansion
- The interplay of electron doping and chemical pressure in Ba(Fe(1-y)Coy)2(As(1-x)Px)2
Cited by in corpus (11)
- Spin fluctuations in iron pnictides and chalcogenides: From antiferromagnetism to superconductivity
- Competing magnetic double-Q phases and superconductivity-induced re-entrance of C2 magnetic stripe order in iron pnictides
- Towards a quantitative description of tunneling conductance of superconductors: application to LiFeAs
- Possible unconventional superconductivity in substituted BaFeAs revealed by magnetic pair-breaking studies
- Fast recovery of the stripe magnetic order by Mn/Fe substitution in F-doped LaFeAsO superconductors
- Superconductivity and phase diagrams of CaK(FeMn)As single crystals
- Effect of proton irradiation on the normal state low-energy excitations of Ba(FeRh)As superconductors
- Scanning tunneling spectroscopy as a probe of multi-Q magnetic states of itinerant magnets
- Competing effects of Mn and Y doping on the low-energy excitations and phase diagram of LaYFeMnAsOF iron-based superconductors
- Magnetic disorder and gap symmetry in optimally electron doped Sr(Fe, Co)As superconductor
- RKKY coupled local moment magnetism in NaFeCuAs