Precise magnetic structure of the low-pressure phase of La3Ni2O7
Determine the exact spin-density-wave magnetic structure of La3Ni2O7 in the low-pressure phase, including ordering wave vectors, layer stacking along the c axis, and moment orientations, and reconcile results from μSR, NMR, RIXS, neutron scattering, and transport.
References
However, the precise magnetic structure of La$_3$Ni$_2$O$_7$ remains under debate.
The dashed line marks an additional density-wave transition ($T_{\text{DW}$), whose origin remains under debate.
The H_{\rm int}(2){\rm M} at the O(2){\rm M} sites could not be experimentally determined, and thus here we tentatively assumed that it is similar to the value at O(3,4) sites.
Although the detailed mechanism is not yet fully understood, this downward shift could be ascribed to the well-developed interlayer spin-singlet formation, which further progresses toward full development upon cooling below T_{\rm SDW}.
Although the charge anomaly at the ideal La(2)a site could not be explicitly observed across T{\rm A} in the previous NQR study, we cannot exclude the possible occurrence of a tiny charge anomaly below T_{\rm A}, which might be associated with the further development of spin-singlet formation upon cooling.
The magnetic structure and the nature of these ordered states remain unclear, as does their relationship to superconductivity.