The tetragonal heavy-fermion superconductor CeRh₂As₂ (Tc=0.3 K) exhibits an exceptionally high critical field of 14 T for B ∥ c. It undergoes a field-driven first-order phase transition between superconducting (SC) states, potentially transitioning from spin-singlet to spin-triplet superconductivity. To elucidate the underlying pairing mechanism, we probe spin fluctuations in CeRh₂As₂ using neutron scattering. We find dynamic (π,π) antiferromagnetic spin correlations with an anisotropic quasi-two-dimensional correlation volume. Our data place an upper limit of 0.31 μB on the staggered magnetization of corresponding N\'{e}el orders at $T=0.08$ K. Density functional theory (DFT) calculations, treating Ce $4f$ electrons as core states, show that the AFM wave vector connects significant areas of the Fermi surface. Our findings show the dominant excitations in CeRh₂As₂ for ω< 1.2~meV are magnetic and indicate superconductivity in CeRh₂As₂ is mediated by AFM spin fluctuations associated with a proximate quantum critical point.
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Chen et al. (2024) studied this question.
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