TY - JOUR
T1 - Toward the Mott state with magnetic cluster formation in heavily Cu-doped NaFe1-xCuxAs
AU - Xin, Yizhou
AU - Stolt, Ingrid
AU - Lee, Jeongseop A.
AU - Song, Yu
AU - Dai, Pengcheng
AU - Halperin, W. P.
PY - 2019/4/8
Y1 - 2019/4/8
N2 - Recent neutron-scattering measurements indicate that NaFe1-xCuxAs forms an antiferromagnetic stripe phase near x≈0.5 in a Mott insulating state. This copper concentration is well in excess of that required for superconductivity, x<0.04. We have investigated the development of magnetism in this compound by using Na23 nuclear magnetic resonance (NMR) spectra and spin-lattice relaxation measurements performed on single crystals (x=0.13, 0.18, 0.24, and 0.39). We find multiple inequivalent Na sites, each of which is associated with a different number of nearest-neighbor Fe sites occupied by a Cu dopant. We show that the distribution of Cu substituted for Fe is random in-plane for low concentrations (x=0.13 and 0.18) but deviates from this with increasing Cu doping. As is characteristic of many pnictide compounds, there is a spin pseudogap that increases in magnitude with dopant concentration. This is correlated with a corresponding increase in orbital NMR frequency shift, indicating a change in valence from Cu2+ to a Cu1+ state as x exceeds 0.18, concomitant with the change of Fe2+ to Fe3+ resulting in the formation of magnetic clusters. However, for x≤0.39 there is no evidence of long-range static magnetic order.
AB - Recent neutron-scattering measurements indicate that NaFe1-xCuxAs forms an antiferromagnetic stripe phase near x≈0.5 in a Mott insulating state. This copper concentration is well in excess of that required for superconductivity, x<0.04. We have investigated the development of magnetism in this compound by using Na23 nuclear magnetic resonance (NMR) spectra and spin-lattice relaxation measurements performed on single crystals (x=0.13, 0.18, 0.24, and 0.39). We find multiple inequivalent Na sites, each of which is associated with a different number of nearest-neighbor Fe sites occupied by a Cu dopant. We show that the distribution of Cu substituted for Fe is random in-plane for low concentrations (x=0.13 and 0.18) but deviates from this with increasing Cu doping. As is characteristic of many pnictide compounds, there is a spin pseudogap that increases in magnitude with dopant concentration. This is correlated with a corresponding increase in orbital NMR frequency shift, indicating a change in valence from Cu2+ to a Cu1+ state as x exceeds 0.18, concomitant with the change of Fe2+ to Fe3+ resulting in the formation of magnetic clusters. However, for x≤0.39 there is no evidence of long-range static magnetic order.
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U2 - 10.1103/PhysRevB.99.155114
DO - 10.1103/PhysRevB.99.155114
M3 - Article
AN - SCOPUS:85064114669
VL - 99
JO - Physical Review B-Condensed Matter
JF - Physical Review B-Condensed Matter
SN - 0163-1829
IS - 15
M1 - 155114
ER -