In iron-based superconductors, high critical temperature () superconductivity over 50 K has only been accomplished in electron-doped FeAsO ( is heavy rare earth () element). Although FeAsO has the highest bulk (58 K), progress in understanding its physical properties has been relatively slow due to difficulties in achieving high-concentration electron doping and carrying out neutron experiments. Here, we present a systematic neutron powder diffraction study of SmFeAsO D , and the discovery of a long-range antiferromagnetic ordering with ≥ 0.56 (AFM2) accompanying a structural transition from tetragonal to orthorhombic. Surprisingly, the Fe magnetic moment in AFM2 reaches a magnitude of 2.73 μ/Fe, which is the largest in all nondoped iron pnictides and chalcogenides. Theoretical calculations suggest that the AFM2 phase originates in kinetic frustration of the Fe-3 orbital, in which the nearest-neighbor hopping parameter becomes zero. The unique phase diagram, i.e., highest- superconducting phase adjacent to the strongly correlated phase in electron-overdoped regime, yields important clues to the unconventional origins of superconductivity.
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http://dx.doi.org/10.1073/pnas.1703295114 | DOI Listing |
Phys Rev Lett
March 2023
Physikalisches Institut, Max-von-Laue-Straße 1, 60438 Frankfurt am Main, Germany.
The nature of the antiferromagnetic order in the heavy fermion metal YbRh_{2}Si_{2}, its quantum criticality, and superconductivity, which appears at low mK temperatures, remain open questions. We report measurements of the heat capacity over the wide temperature range 180 μK-80 mK, using current sensing noise thermometry. In zero magnetic field we observe a remarkably sharp heat capacity anomaly at 1.
View Article and Find Full Text PDFProc Natl Acad Sci U S A
May 2021
Department of Physics, University of California San Diego, La Jolla, CA 92093;
Electrical resistivity measurements were performed on single crystals of URu Os Si up to = 0.28 under hydrostatic pressure up to = 2 GPa. As the Os concentration, , is increased, 1) the lattice expands, creating an effective negative chemical pressure (); 2) the hidden-order (HO) phase is enhanced and the system is driven toward a large-moment antiferromagnetic (LMAFM) phase; and 3) less external pressure is required to induce the HO→LMAFM phase transition.
View Article and Find Full Text PDFJ Phys Condens Matter
November 2018
Centro Brasileiro de Pesquisas Físicas, Rua Dr. Xavier Sigaud, 150-Urca, Rio de Janeiro-RJ 22290-180, Brazil.
In this work, we introduce the Heisenberg Ising-Kondo necklace with transverse field as a possible model to describe the heavy-fermion compound URuSi. The physics of this compound presents many open questions, like the transition to the hidden order (HO) phase at T = 17.5 K.
View Article and Find Full Text PDFSci Rep
September 2017
II. Physikalisches Institut, Universität zu Köln, Zülpicher Str. 77, D-50937, Köln, Germany.
Two strong arguments in favor of magnetically driven unconventional superconductivity arise from the coexistence and closeness of superconducting and magnetically ordered phases on the one hand, and from the emergence of magnetic spin-resonance modes at the superconducting transition on the other hand. Combining these two arguments one may ask about the nature of superconducting spin-resonance modes occurring in an antiferromagnetic state. This problem can be studied in underdoped BaFe As, for which the local coexistence of large moment antiferromagnetism and superconductivity is well established by local probes.
View Article and Find Full Text PDFProc Natl Acad Sci U S A
September 2017
Department of Physics, University of California, San Diego, La Jolla, CA 92093;
Electrical transport measurements were performed on URu Fe Si single-crystal specimens in high magnetic fields up to 45 T (DC fields) and 60 T (pulsed fields). We observed a systematic evolution of the critical fields for both the hidden-order (HO) and large-moment antiferromagnetic (LMAFM) phases and established the 3D phase diagram of In the HO phase, / scales with / and collapses onto a single curve. However, in the LMAFM phase, this single scaling relation is not satisfied.
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