Journal
PHYSICAL REVIEW B
Volume 103, Issue 18, Pages -Publisher
AMER PHYSICAL SOC
DOI: 10.1103/PhysRevB.103.L180506
Keywords
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Funding
- Deutsche Forschungsgemeinschaft (DFG) [AS 523/4-1, DI2538/1-1, GRK1621, SFB 1143, 247310070]
- Wurzburg-Dresden Cluster of Excellence on Complexity and Topology in Quantum Matter ct.qmat [EXC 2147, 390858490]
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The phase diagram of LaFe1-xCoxAsO single crystals was determined using nuclear magnetic resonance (NMR). The results showed that F-doped samples exhibit superconductivity at low doping levels, while Co-doped samples exhibit structural and magnetic transitions. Short-range magnetic order was observed at doping levels up to x = 0.056, and magnetic fluctuations revealed the interplay of nematicity and magnetism.
We determine the phase diagram of LaFe1-xCoxAsO single crystals by using nuclear magnetic resonance (NMR). Up to a nominal doping of x = 0.03, it follows the phase diagram for F-doped polycrystals. Above x = 0.03, the F-doped samples become superconducting, whereas for Co doping the structural and magnetic transitions can be observed up to x = 0.042, and superconductivity occurs only for higher doping levels and with reduced transition temperatures. For dopings up to x = 0.056, we find evidence for short-range magnetic order. By means of relaxation-rate measurements, we map out the magnetic fluctuations that reveal the interplay of nematicity and magnetism. Above the nematic ordering, the spin fluctuations in LaFe1-xCoxAsO are identical to those in Ba(Fe1-xCox)(2)As-2, suggesting that nematicity in LaFeAsO is a result of the fluctuating spin density wave as well.
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