Multipolar fluctuation calculations support antiferromagnetic order at wavevector (1/2,1/2,0) as the origin of the non-superconducting phase in CeRh2As2.
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Multipolar fluctuations from localized 4f electrons in CeRh2As2
Multipolar fluctuation calculations support antiferromagnetic order at wavevector (1/2,1/2,0) as the origin of the non-superconducting phase in CeRh2As2.