Duan Chunruo, Sasmal Kalyan, Maple M Brian, Podlesnyak Andrey, Zhu Jian-Xin, Si Qimiao, Dai Pengcheng
Department of Physics and Astronomy, Rice Center for Quantum Materials, Rice University, Houston, Texas 77005, USA.
Department of Physics, University of California, San Diego, California 92093, USA.
Phys Rev Lett. 2020 Dec 4;125(23):237003. doi: 10.1103/PhysRevLett.125.237003.
Spin-triplet superconductors are of extensive current interest because they can host topological state and Majorana fermions important for quantum computation. The uranium-based heavy-fermion superconductor UTe_{2} has been argued as a spin-triplet superconductor similar to UGe_{2}, URhGe, and UCoGe, where the superconducting phase is near (or coexists with) a ferromagnetic (FM) instability and spin-triplet electron pairing is driven by FM spin fluctuations. Here we use neutron scattering to show that, although UTe_{2} exhibits no static magnetic order down to 0.3 K, its magnetism in the [0,K,L] plane is dominated by incommensurate spin fluctuations near an antiferromagnetic ordering wave vector and extends to at least 2.6 meV. We are able to understand the dominant incommensurate spin fluctuations of UTe_{2} in terms of its electronic structure calculated using a combined density-functional and dynamic mean-field theory.
自旋三重态超导体目前备受关注,因为它们能够承载对量子计算至关重要的拓扑态和马约拉纳费米子。铀基重费米子超导体UTe₂被认为是一种类似于UGe₂、URhGe和UCoGe的自旋三重态超导体,其超导相接近(或与)铁磁(FM)不稳定性共存,且自旋三重态电子配对由FM自旋涨落驱动。在此,我们利用中子散射表明,尽管UTe₂在低至0.3 K时未表现出静态磁序,但其在[0,K,L]平面内的磁性主要由反铁磁有序波矢附近的非公度自旋涨落主导,且延伸至至少2.6 meV。我们能够根据使用密度泛函和动态平均场理论相结合计算出的电子结构,理解UTe₂中占主导地位的非公度自旋涨落现象。