2021
DOI: 10.1038/s42005-021-00621-4
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Magnetic and f-electron effects in LaNiO2 and NdNiO2 nickelates with cuprate-like $$3{d}_{{x}^{2}-{y}^{2}}$$ band

Abstract: Recent discovery of superconductivity in the doped infinite-layer nickelates has renewed interest in understanding the nature of high-temperature superconductivity more generally. The low-energy electronic structure of the parent compound NdNiO2, the role of electronic correlations in driving superconductivity, and the possible relationship between the cuprates and the nickelates are still open questions. Here, by comparing LaNiO2 and NdNiO2 systematically within a parameter-free, all-electron first-principles… Show more

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Cited by 57 publications
(33 citation statements)
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“…Neél type order is consistently obtained in DFT studies [24, 27, 29, and 51], as in d 9 insulating cuprates. The predicted AFM ground state in DFT + U calculations [64] is characterized by the involvement of both d x 2 −y 2 and d z 2 Ni bands [65]. This state is peculiar in that it displays a flat-band one-dimensional-like van Hove singularity of d z 2 character pinned at the Fermi level.…”
Section: From ∞mentioning
confidence: 96%
“…Neél type order is consistently obtained in DFT studies [24, 27, 29, and 51], as in d 9 insulating cuprates. The predicted AFM ground state in DFT + U calculations [64] is characterized by the involvement of both d x 2 −y 2 and d z 2 Ni bands [65]. This state is peculiar in that it displays a flat-band one-dimensional-like van Hove singularity of d z 2 character pinned at the Fermi level.…”
Section: From ∞mentioning
confidence: 96%
“…Theoretically a number of DFT + U, hybrid DFT and DFT + DMFT studies have studied magnetism of infinite layer nickelates [17,21,24,25,84,99,101,108,111] and reported a wide range of magnetic superexchange [17,18,23,66,76,77,99,112] from a small value of about 10 meV [23,99] to an intermediate value of about 30 meV [66] to a large value of about 80-100 meV [17,18,76,77,112]. DFT + DMFT studies have not examined the Ni 13 MLWF 2 U = 7, J = 0.7 290 7.6 [44] 13 SLWF 2 U = 7, J = 0.7 290 3.9 [117] 16 MLWF (Ni, Nd, O) 5 U avg = 6, J avg = 0.95 290 3 [44] Projectors −10 to 3 2 U = 7, J = 0.7 290 5.6 [108] Projectors −10 to 3 5 U avg = 10, J avg = 1 30 6.4 [108] Projectors −10 to 3 5 U avg = 10, J avg = 1 (SIC on O) 30 Mott insulating [44] Projectors −10 to 10 2 U = 7, J = 0.7 290 4.6 [27] Projectors −10 to 10 5 U avg = 7, J avg = 0.7 390 3.7 [16] Projectors −10 to 10 5 U avg = 5, J avg = 1 100 2.8 [101] Projectors −10 to 10 5 U avg = 5, J avg = 0.8 -2.4 [101] Projectors −10 to 10 5 U avg = 9, J avg = 0.8 -4.1 [15] Projectors −10 to 10 exchange coupling systematically.…”
Section: Magnetismmentioning
confidence: 99%
“…Neél type order is consistently obtained in DFT studies 24,27,29,51 , as in d 9 insulating cuprates. The predicted AFM ground state in DFT+U calculations 61 is characterized by the involvement of both d x 2 −y 2 and d z 2 Ni bands 62 . This state is peculiar in that it displays a flat-band one-dimensional-like van Hove singularity of d z 2 character pinned at the Fermi level.…”
Section: Introductionmentioning
confidence: 98%