Strongly Correlated Spin Research Team

Study of relationship between magnetism and mechanism of superconductivity in Ce(Co,Rh)In₅

CeCoIn₅ has attracted particular attention among f-electron unconventional superconductors because of the existence of resonance peaks, FFLO phases, and anomalous quasiparticles that appear in the superconducting phase. In addition, since there is a quantum critical point associated with the antiferromagnetically ordered phase in the vicinity, magnetic fluctuations are expected to contribute to the mechanism of its superconductivity. So far, we have succeeded in identifying the Fermi surface that contributes to the superconductivity of CeCoIn₅ based on the results of neutron diffraction experiments on Ce(Rh,Co)In₅, and have reported that the magnetic form factor in this system shows almost no magnetic field dependence in the high magnetic field region by small angle neutron scattering experiments. In this fiscal year, we further tried to investigate the interaction between magnetism and superconductivity in CeCoIn₅ by following the resonance peaks in CeRh_0.2Co_0.8In₅ by inelastic neutron scattering experiments, and found a new magnetic ordered phase. We need to investigate further this phase to reveal the mechanism of superconductivity in CeCoIn₅ in detail.

Magnetic scattering observed along (0.5 0.5 L) at 0.7K.

Contribution of phonon excitations to the superconducting mechanism of non-centrosymmetric LaNiC₂

LaNiC₂ is a superconductor (T_c = 2.7K) without spatial inversion symmetry. Theoretical group predicted that the phonon dispersion of this material may show kohn anomalies. In rare earth-nickel-boron-carbide superconductors (eg RENi₂B₂C), not only a kohn-anomaly but also resonance like peaks are observed at a specific q position, where nesting of the Fermi surface is expected to occur. To verify the possibility of both kohn-anomaly and resonance behaviors and to study their contribution to the mechanism of its superconductivity, we performed neutron scattering experiments. It was impossible to carry out a new experiment in FY 2020, we proceeded to analyze previous data measured by the high-resolution chopper spectroscope HRC in the J-PARC MLF of the Japan Atomic Energy Agency (JAEA). The results revealed longitudinal and transverse acoustic phonon branches. It was also clarified that a certain amount of phonon spectral was observed on the higher energy side but the intensity was too weak to identify the dispersion relation. We plan to conduct a new inelastic neutron scattering experiment in the experimental reactor JRR-3 at JAEA to draw the whole picture of the dispersion relation of the lattice fluctuation of this system.

Phonon excitation spectrum in a range of 7<E<9 meV at 300K and in the (H0L) scattering plane.

Superconducting mechanism and magnetic fluctuations in CeRh_0.6Co_0.4In₅

CeCoIn₅ has attracted much attention, since it shows several interesting phenomena, including a resonance magnetic peak, which appears below the superconducting transition temperature, Tc, a SDW magnetic order, a so-called “Q phase”, that is stabilized only in the superconducting phase. In this study, in order to clarify the relationship between magnetism and superconductivity, we performed inelastic neutron scattering experiments on CeRh_0.6Co_0.4In₅. Resonance peaks accompanying the superconducting transition were not detected, but spin wave excitation appeared below T_N along (1/2 1/2 l).

An analysis of the energy dependence of the excitation revealed that the dispersion relation in the [h h 0] direction is nearly independent of l. This suggests that there is a two-dimensional spin correlation in this system.

Energy dispersion curve of magnetic excitations observed along (1/2 1/2 l)

SANS experiment on beta−PdBi₂ superconductor

For topological superconductors, special particles, so-called Majorana fermions, are predicted to appear on the surface of the material. We studied a candidate material of topological superconductors, β-PdBi₂ (space group I4/mmm, T_c = 5.4 K), to bare its bulk properties including superconducting symmetry and gap structures by specific heat and small angle neutron scattering (SANS) measurements. For the present study, we succeeded in growing single crystals of β-PdBi₂ by a melt growth method and T_c of the crystals was evaluated to be T_c = 5.2 K by magnetization measurements. Temperature dependence of neutron diffraction intensities originated from vortex lattice suggests that topological superconductor β-PdBi₂ has an anisotropic superconducting full-gap. Moreover, we succeeded in revealing that the energy value of anisotropic full-gap estimated from small-angle neutron scattering experiments can reproduce the temperature dependence of electric heat capacity.

Temperature dependence of vortex Bragg diffraction of β-PdBi₂.