TY - JOUR
T1 - Spin fluctuations in Sr1.8La0.2RuO4
AU - He, Zheng
AU - Wang, Qisi
AU - Feng, Yu
AU - Kim, Chul
AU - Kyung, Wonshik
AU - Kim, Changyoung
AU - Wo, Hongliang
AU - Ding, Gaofeng
AU - Hao, Yiqing
AU - Liu, Feiyang
AU - Walker, Helen C.
AU - Adroja, Devashibhai T.
AU - Schneidewind, Astrid
AU - Wang, Wenbin
AU - Zhao, Jun
N1 - Publisher Copyright:
© 2023 American Physical Society.
PY - 2023/5/15
Y1 - 2023/5/15
N2 - We use inelastic neutron scattering to study spin fluctuations in Sr1.8La0.2RuO4, where Lanthanum doping triggers a Lifshitz transition by pushing the van Hove singularity in the γ band to the Fermi energy. Strong spin fluctuations emerge at an incommensurate wave vector Qic=(0.3,0.3), corresponding to the nesting vector between α and β Fermi sheets. The incommensurate antiferromagnetic fluctuations shift toward (0.25,0.25) with increasing energy up to ∼110 meV. By contrast, scatterings near the ferromagnetic wave vectors Q=(1,0) and (1,1) remain featureless at all energies. This contradicts the weak-coupling perspective that suggests a sharp enhancement of ferromagnetic susceptibility due to the divergence of density of states in the associated γ band. Our findings imply that ferromagnetic fluctuations in Sr2RuO4 and related materials do not fit into the weak-coupling paradigm, but instead are quasilocal fluctuations induced by Hund's coupling. This imposes significant constraints for the pairing mechanism involving spin fluctuations.
AB - We use inelastic neutron scattering to study spin fluctuations in Sr1.8La0.2RuO4, where Lanthanum doping triggers a Lifshitz transition by pushing the van Hove singularity in the γ band to the Fermi energy. Strong spin fluctuations emerge at an incommensurate wave vector Qic=(0.3,0.3), corresponding to the nesting vector between α and β Fermi sheets. The incommensurate antiferromagnetic fluctuations shift toward (0.25,0.25) with increasing energy up to ∼110 meV. By contrast, scatterings near the ferromagnetic wave vectors Q=(1,0) and (1,1) remain featureless at all energies. This contradicts the weak-coupling perspective that suggests a sharp enhancement of ferromagnetic susceptibility due to the divergence of density of states in the associated γ band. Our findings imply that ferromagnetic fluctuations in Sr2RuO4 and related materials do not fit into the weak-coupling paradigm, but instead are quasilocal fluctuations induced by Hund's coupling. This imposes significant constraints for the pairing mechanism involving spin fluctuations.
UR - http://www.scopus.com/inward/record.url?scp=85159660458&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.107.L201107
DO - 10.1103/PhysRevB.107.L201107
M3 - Article
AN - SCOPUS:85159660458
SN - 2469-9950
VL - 107
JO - Physical Review B
JF - Physical Review B
IS - 20
M1 - L201107
ER -