Resonance from antiferromagnetic spin fluctuations for superconductivity in UTe2
Resonance from antiferromagnetic spin fluctuations for superconductivity in UTe2
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DOI:
10.1038/s41586-021-04151-5
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发表时间:
2021-12-23
期刊:
影响因子:
64.8
通讯作者:
Dai, Pengcheng
中科院分区:
文献类型:
--
作者:
Duan, Chunruo;Baumbach, R. E.;Dai, Pengcheng
Superconductivity originates from the formation of bound (Cooper) pairs of electrons that can move through the lattice without resistance below the superconducting transition temperature T-c (ref. (1)). Electron Cooper pairs in most superconductors form anti-parallel spin singlets with total spin S = 0 (ref. (2)), although they can also form parallel spin-triplet Cooper pairs with S = 1 and an odd parity wavefunction(3). Spin-triplet pairing is important because it can host topological states and Majorana fermions relevant for quantum computation(4,5). Because spin-triplet pairing is usually mediated by ferromagnetic (FM) spin fluctuations(3), uranium-based materials near an FM instability are considered to be ideal candidates for realizing spin-triplet superconductivity(6). Indeed, UTe2, which has a T-c approximate to 1.6 K (refs.(7,8)), has been identified as a candidate for a chiral spin-triplet topological superconductor near an FM instability(7-14), although it also has antiferromagnetic (AF) spin fluctuations(15,16). Here we use inelastic neutron scattering (INS) to show that superconductivity in UTe2 is coupled to a sharp magnetic excitation, termed resonance(17-23), at the Brillouin zone boundary near AF order. Because the resonance has only been found in spin-singlet unconventional superconductors near an AF instability(17-23), its observation in UTe2 suggests that AF spin fluctuations may also induce spin-triplet pairing(24) or that electron pairing in UTe2 has a spin-singlet component.