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Electronic and Magnetic Structures of Hole Doped Trilayer La<sub>4–<i>x</i></sub>Sr<sub><i>x</i></sub>Ni<sub>3</sub>O<sub>8</sub>from First-Principles Calculations

12

Citations

30

References

2016

Year

Abstract

The magnetic and electronic properties of trilayer La<sub>4</sub>Ni<sub>3</sub>O<sub>8</sub>, similar to hole-doped cuprates, are investigated by performing full-potential linearized augmented plane wave method-based spin-polarized calculations with LDA and GGA functionals including Hubbard U parameters to account for strong correlation effects. On the basis of these calculations, we found that La<sub>4</sub>Ni<sub>3</sub>O<sub>8</sub> is a C-type anti-ferromagnetic (C-AFM) Mott insulator in agreement with previous experimental and theoretical observations. Our calculations suggest that the two crystallographically nonequivalent nickel atoms Ni1 and Ni2 are found to be in high-spin state with an average valency of +1.33. Intermediate band-gap states are originated from d<sub>z<sup>2</sup></sub> electrons of both types of Ni ions after including the strong correlation effects. To understand the role of hole doping on electronic structure, phase stability, and magnetic properties of La<sub>4</sub>Ni<sub>3</sub>O<sub>8</sub>, similar calculations were performed for La<sub>4-x</sub>Sr<sub>x</sub>Ni<sub>3</sub>O<sub>8</sub> as a function of x, using the supercell approach. We found that the hole doping brings insulator-to-metal transition without changing the C-AFM ordering, though the magnetic moment is enhanced at both Ni sites. Moreover, these Ni atoms are always in an average valence state irrespective of hole doping or volume change. So the electronic properties of hole-doped La<sub>4</sub>Ni<sub>3</sub>O<sub>8</sub> cannot be compared with hole-doped cuprates that are high-T<sub>C</sub> superconductors.

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