| Autor: |
Myung-Chul Jung, Harrison LaBollita, Victor Pardo, Antia S. Botana |
| Jazyk: |
angličtina |
| Rok vydání: |
2022 |
| Předmět: |
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| Zdroj: |
Scientific Reports, Vol 12, Iss 1, Pp 1-9 (2022) |
| Druh dokumentu: |
article |
| ISSN: |
2045-2322 |
| DOI: |
10.1038/s41598-022-22176-2 |
| Popis: |
Abstract We provide a set of computational experiments based on ab initio calculations to elucidate whether a cuprate-like antiferromagnetic insulating state can be present in the phase diagram of the low-valence layered nickelate family (R $$_{n+1}$$ n + 1 Ni $$_n$$ n O $$_{2n+2}$$ 2 n + 2 , R= rare-earth, $$n=1-\infty$$ n = 1 - ∞ ) in proximity to half-filling. It is well established that at $$d^9$$ d 9 filling the infinite-layer ( $$n=\infty$$ n = ∞ ) nickelate is metallic, in contrast to cuprates wherein an antiferromagnetic insulator is expected. We show that for the Ruddlesden-Popper (RP) reduced phases of the series (finite n) an antiferromagnetic insulating ground state can naturally be obtained instead at $$d^9$$ d 9 filling, due to the spacer RO $$_2$$ 2 fluorite slabs present in their structure that block the c-axis dispersion. In the $$n=\infty$$ n = ∞ nickelate, the same type of solution can be derived if the off-plane R-Ni coupling is suppressed. We show how this can be achieved if a structural element that cuts off the c-axis dispersion is introduced (i.e. vacuum in a monolayer of RNiO $$_2$$ 2 , or a blocking layer in multilayers formed by (RNiO $$_2$$ 2 ) $$_1$$ 1 /(RNaO $$_2$$ 2 ) $$_1$$ 1 ). |
| Databáze: |
Directory of Open Access Journals |
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