TY - JOUR
T1 - Out-of-plane magnetic phase diagram of the Kitaev quantum magnet Na2Co2TeO6
AU - Zhang, Shengzhi
AU - Lee, Sangyun
AU - Brosha, Eric
AU - Huang, Qing
AU - Zhou, Haidong
AU - Zapf, Vivien S.
AU - Lee, Minseong
PY - 2024/10/1
Y1 - 2024/10/1
N2 - We have investigated the magnetic properties and mapped out the phase diagram of the honeycomb magnet Na2Co2TeO6 with Co 3d7 in out-of-plane magnetic fields. This material has previously been proposed to show nearest-neighbor Kitaev interactions between Co spins and maybe even Kitaev quantum spin liquid behavior in high fields. At 0.01 T, we observe a thermal phase transition at TN=27K, transitioning from a paramagnetic state to a canonical ferrimagnetic state. Upon increasing the magnetic field, a spin-floplike phase transition occurred before saturation of J=1/2 between 10 K and TN. Below 10 K, a peak-dip-peak structure emerges between 10 and 17 T in the magnetic susceptibility (dM/dH) before the magnetic saturation, reminiscent of magnetization plateau behavior. The measurement of the magnetocaloric effect also shows dip-peak-dip behavior in this field range. Our data can be explained by an XXZ model with a single ion anisotropy and possibly small Kitaev and Γ exchange interactions. We also determined the magnetization saturation field that helps constrain the energy scale of the exchange interactions.
AB - We have investigated the magnetic properties and mapped out the phase diagram of the honeycomb magnet Na2Co2TeO6 with Co 3d7 in out-of-plane magnetic fields. This material has previously been proposed to show nearest-neighbor Kitaev interactions between Co spins and maybe even Kitaev quantum spin liquid behavior in high fields. At 0.01 T, we observe a thermal phase transition at TN=27K, transitioning from a paramagnetic state to a canonical ferrimagnetic state. Upon increasing the magnetic field, a spin-floplike phase transition occurred before saturation of J=1/2 between 10 K and TN. Below 10 K, a peak-dip-peak structure emerges between 10 and 17 T in the magnetic susceptibility (dM/dH) before the magnetic saturation, reminiscent of magnetization plateau behavior. The measurement of the magnetocaloric effect also shows dip-peak-dip behavior in this field range. Our data can be explained by an XXZ model with a single ion anisotropy and possibly small Kitaev and Γ exchange interactions. We also determined the magnetization saturation field that helps constrain the energy scale of the exchange interactions.
UR - http://www.scopus.com/inward/record.url?scp=85207359533&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.110.144431
DO - 10.1103/PhysRevB.110.144431
M3 - Article
SN - 1098-0121
VL - 110
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 14
M1 - 144431
ER -