2022
Exchange interactions in d5 Kitaev materials: From Na2IrO3 to α−RuCl3
LIU, Huimei; Jiří CHALOUPKA a Giniyat KHALIULLINZákladní údaje
Originální název
Exchange interactions in d5 Kitaev materials: From Na2IrO3 to α−RuCl3
Autoři
LIU, Huimei; Jiří CHALOUPKA a Giniyat KHALIULLIN
Vydání
Physical Review B, American Physical Society, 2022, 2469-9950
Další údaje
Jazyk
angličtina
Typ výsledku
Článek v odborném periodiku
Obor
10302 Condensed matter physics
Stát vydavatele
Spojené státy
Utajení
není předmětem státního či obchodního tajemství
Odkazy
Impakt faktor
Impact factor: 3.700
Označené pro přenos do RIV
Ano
Kód RIV
RIV/00216224:14310/22:00129107
Organizační jednotka
Přírodovědecká fakulta
UT WoS
EID Scopus
Klíčová slova anglicky
Exact diagonalization; Kitaev model; Honeycomb lattice; Strongly correlated systems; Magnetic interactions; Magnetism; Magnons; Spin liquid
Příznaky
Mezinárodní význam, Recenzováno
Změněno: 5. 12. 2022 11:29, Mgr. Marie Novosadová Šípková, DiS.
Anotace
V originále
We present an analytical study of the exchange interactions between pseudospin one-half d5 ions in honeycomb lattices with edge-shared octahedra. Various exchange channels involving Hubbard U, charge-transfer excitations, and cyclic exchange are considered. Hoppings within t2g orbitals as well as between t2g and eg orbitals are included. Special attention is paid to the trigonal crystal field Δ effects on the exchange parameters. The obtained exchange Hamiltonian is dominated by ferromagnetic Kitaev interaction K within a wide range of Δ. It is found that a parameter region close to the charge-transfer insulator regime and with a small Δ is most promising to realize the Kitaev spin liquid phase. Two representative honeycomb materials Na2IrO3 and α-RuCl3 are discussed based on our theory. We have found that both materials share dominant ferromagnetic K and positive nondiagonal Γ values. However, their Heisenberg J terms have opposite signs: AFM J>0 in Na2IrO3 and FM J<0 in α-RuCl3. This brings different magnetic fluctuations and results in their different magnetization behaviors and spin excitation spectra. Proximity to FM state due to the large FM J is emphasized in α-RuCl3. The differences between the exchange couplings of these two materials originate from the opposite Δ values, indicating that the crystal field can serve as an efficient control parameter to tune the magnetic properties of d5 spin-orbit Mott insulators.
Návaznosti
| GA19-16937S, projekt VaV |
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