TY - JOUR
T1 - Effect of isoelectronic doping on the honeycomb-lattice iridate A2 IrO3
AU - Manni, S.
AU - Choi, Sungkyun
AU - Mazin, I. I.
AU - Coldea, R.
AU - Altmeyer, Michaela
AU - Jeschke, Harald O.
AU - Valentí, Roser
AU - Gegenwart, P.
PY - 2014/6/11
Y1 - 2014/6/11
N2 - We have investigated, experimentally and theoretically, the series (Na1-xLix)2IrO3. Contrary to what has been believed so far, only for x≤0.25 does the system form uniform solid solutions where Li preferentially goes to the Ir2Na planes, as observed in our density functional theory calculations and consistent with x-ray diffraction analysis. For larger Li content, as evidenced by powder x-ray diffraction, scanning electron microscopy, and density functional theory calculations, the system shows a miscibility gap and a phase separation into an ordered Na3LiIr2O6 phase with alternating Na3 and LiIr2O6 planes, and a Li-rich phase close to pure Li2IrO3. For x≤0.25 we observe (1) an increase of c/a with Li doping up to x=0.25, despite the fact that c/a in pure Li2IrO3 is smaller than in Na2IrO3, and (2) a gradual reduction of the antiferromagnetic ordering temperature TN and ordered moment. In view of our results showing clear evidence for phase separation for 0.25≤x≤0.6, more detailed studies are needed to confirm the presence or absence of phase separation at the higher doping x∼0.7, where a continuum quantum phase transition has been proposed previously.
AB - We have investigated, experimentally and theoretically, the series (Na1-xLix)2IrO3. Contrary to what has been believed so far, only for x≤0.25 does the system form uniform solid solutions where Li preferentially goes to the Ir2Na planes, as observed in our density functional theory calculations and consistent with x-ray diffraction analysis. For larger Li content, as evidenced by powder x-ray diffraction, scanning electron microscopy, and density functional theory calculations, the system shows a miscibility gap and a phase separation into an ordered Na3LiIr2O6 phase with alternating Na3 and LiIr2O6 planes, and a Li-rich phase close to pure Li2IrO3. For x≤0.25 we observe (1) an increase of c/a with Li doping up to x=0.25, despite the fact that c/a in pure Li2IrO3 is smaller than in Na2IrO3, and (2) a gradual reduction of the antiferromagnetic ordering temperature TN and ordered moment. In view of our results showing clear evidence for phase separation for 0.25≤x≤0.6, more detailed studies are needed to confirm the presence or absence of phase separation at the higher doping x∼0.7, where a continuum quantum phase transition has been proposed previously.
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U2 - 10.1103/PhysRevB.89.245113
DO - 10.1103/PhysRevB.89.245113
M3 - Article
AN - SCOPUS:84902839205
SN - 1098-0121
VL - 89
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 24
M1 - 245113
ER -