Anisotropic excitonic magnetism from discrete $\mathrm{C}_{4}$ symmetry in CeRhIn$_{5}$

TL;DR

This study investigates the anisotropic magnetic excitations in CeRhIn$_{5}$ using neutron spectroscopy and a crystal field model, revealing tunable anisotropy and multi-level effects constrained by C4 symmetry.

Contribution

The paper develops a methodology combining crystal field Hamiltonian diagonalization and RPA to analyze anisotropic excitations in CeRhIn$_{5}$, highlighting the importance of multi-level states and symmetry constraints.

Findings

Identified two polarized magnetic modes along c and a-b planes.

Demonstrated the tunability of anisotropy and excitation bandwidth with magnetic field.

Showed the instability of in-plane polarized excitations in CeRhIn$_{5}$.

Abstract

Anisotropy in strongly correlated materials is a central parameter in determining the electronic ground state and is tuned through the local crystalline electric field. This is notably the case in the CeCo$_{x}$Rh$_{1-x}$In$_{5}$ system where the ground-state wave function can provide the basis for antiferromagnetism and/or unconventional superconductivity. We develop a methodology to understand the local magnetic anisotropy and experimentally investigate with neutron spectroscopy applied to antiferromagnetic ($T_{N}$=3.8 K) CeRhIn$_{5}$ which is isostructural to $d$-wave superconducting ($T_{c}$=2.3 K) CeCoIn$_{5}$. Through diagonalizing the local crystal field Hamiltonian with discrete tetragonal $\mathrm{C}_{4}$ point group symmetry and coupling these states with the Random Phase Approximation (RPA), we find two distinct modes polarized along the crystallographic $c$ and $a-b$ planes, agreeing with experiment. The anisotropy and bandwidth, underlying the energy scale of these modes, are tuneable with a magnetic field which we use experimentally to separate in energy single and multiparticle excitations thereby demonstrating the instability of excitations polarized within the crystallographic $a-b$ plane in CeRhIn$_{5}$. We compare this approach to a $S_{eff}={1\over 2}$ parameterizations and argue for the need to extend conventional SU(2) theories of magnetic excitations to utilize the multi-level nature of the underlying crystal-field basis states constrained by the local point-group $\mathrm{C}_{4}$ symmetry.