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Volumn 85, Issue 21, 2012, Pages

Ab initio study of the factors affecting the ground state of rare-earth nickelates

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EID: 84863319054     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.85.214431     Document Type: Article
Times cited : (22)

References (35)
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    • We also found that a rather different solution, metallic and with a large net magnetization, is the predicted ground state of bulk NNO when using U values above 3 eV. Thus, for our chosen value of U = 7 eV, the calculations actually predict a ground state that is in clear disagreement with the experimental observations, and we should deem the present work as restricted to spin configurations that resemble the experimentally observed phases, which have essentially zero remnant magnetization.
    • We also found that a rather different solution, metallic and with a large net magnetization, is the predicted ground state of bulk NNO when using U values above 3 eV. Thus, for our chosen value of U = 7 eV, the calculations actually predict a ground state that is in clear disagreement with the experimental observations, and we should deem the present work as restricted to spin configurations that resemble the experimentally observed phases, which have essentially zero remnant magnetization.
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    • The breathing mode corresponds to the R point of the Brillouin zone of the ideal five-atom perovskite cell, while the JT distortion is associated to the M point.
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    • The scheme employed to estimate atomic charges tends to render values that are too small, as evidenced by the fact that the sum of the electronic charges assigned to all the atoms does not reach the total number of electrons. Further, the hybridization between Ni and O orbitals is clearly very large in these nickelates. As a result of these two factors, the estimated ionization states deviate significantly from the nominal ones that would correspond to the ionic limit. Thus, here we only report charge differences, which are of greater physical significance than the values obtained for individual atomic charges.
    • The scheme employed to estimate atomic charges tends to render values that are too small, as evidenced by the fact that the sum of the electronic charges assigned to all the atoms does not reach the total number of electrons. Further, the hybridization between Ni and O orbitals is clearly very large in these nickelates. As a result of these two factors, the estimated ionization states deviate significantly from the nominal ones that would correspond to the ionic limit. Thus, here we only report charge differences, which are of greater physical significance than the values obtained for individual atomic charges.
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    • 2 does not imply that all Ni atoms are crystallographically equivalent. In fact, for all Ni's to be equivalent, we would need to have a perfect Pnma symmetry, which we never observed.
    • 2 does not imply that all Ni atoms are crystallographically equivalent. In fact, for all Ni's to be equivalent, we would need to have a perfect P n m a symmetry, which we never observed.
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    • To determine the symmetry of our relaxed structures, we used the program findsym
    • To determine the symmetry of our relaxed structures, we used the program findsym [H. T. Stokes and D. M. Hatch (2004), http://stokes.byu.edu/isotropy. html] employing a value of 0.01 Å for the accuracy within which atomic positions and lattice vectors are known.
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    • For bulk NNO and U = 7 eV, we obtain a pseudocubic in-plane lattice constant of about 3.87 Å. Experimentally, the pseudocubic in-plane lattice constant of NNO is about 5.38/√2 Å = 3.80 Å, as derived from the results of Ref. at 50 K.
    • For bulk NNO and U = 7 eV, we obtain a pseudocubic in-plane lattice constant of about 3.87 Å. Experimentally, the pseudocubic in-plane lattice constant of NNO is about 5.38/ √ 2 Å = 3.80 Å, as derived from the results of Ref. at 50 K.
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    • This would correspond to the strong-coupling limit discussed in, PRBMDO 1098-0121 10.1103/PhysRevB.84.165119
    • This would correspond to the strong-coupling limit discussed in S. B. Lee, R. Chen, and L. Balents, Phys. Rev. B PRBMDO 1098-0121 10.1103/PhysRevB.84. 165119 84, 165119 (2011).
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    • 3 as relying on a type of Fermi-nesting mechanism that is usually associated with weak correlations
    • 3 as relying on a type of Fermi-nesting mechanism that is usually associated with weak correlations.
    • Mazin1    Lee2


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