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.
N1 - Funding Information:
We thank Arneil Reyes for use of facilities at NHMFL, and Weiyi Wang and Chongde Cao for their contributions to the crystal growth and characterization. Research was supported by the U.S. Department of Energy (DOE), Office of Basic Energy Sciences (BES), Division of Material Sciences and Engineering under Award No. DE-FG02-05ER46248 (W.P.H.) and DE-FG02-05ER46202 (P.D.), and the NHMFL by NSF and the State of Florida. The single crystal growth efforts at Rice were supported by the U.S. DOE, BES under Grant No. DE-SC0012311. Part of the materials work at Rice was supported by the Robert A. Welch Foundation under Grant No. C-1839.
Funding Information:
We thank Arneil Reyes for use of facilities at NHMFL, and Weiyi Wang and Chongde Cao for their contributions to the crystal growth and characterization. Research was supported by the U.S. Department of Energy (DOE), Office of Basic Energy Sciences (BES), Division of Material Sciences and Engineering under Award No. DE-FG02-05ER46248 (W.P.H.) and DE-FG02-05ER46202 (P.D.), and the NHMFL by NSF and the State of Florida. The single crystal growth efforts at Rice were supported by the U.S. DOE, BES under Grant No. DE-SC0012311. Part of the materials work at Rice was supported by the Robert A. Welch Foundation under Grant No. C-1839.
Publisher Copyright:
© 2019 American Physical Society.
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 -