4.8 Article

Stacked charge stripes in the quasi-2D trilayer nickelate La4Ni3O8

Publisher

NATL ACAD SCIENCES
DOI: 10.1073/pnas.1606637113

Keywords

charge stripe; charge order; nickelate; strongly correlated materials; transition metal oxides

Funding

  1. US Department of Energy, Office of Science, Basic Energy Sciences, Materials Science and Engineering Division
  2. Divisions of Chemistry (CHE) and Materials Research (DMR), National Science Foundation [NSF/CHE-1346572]
  3. US DOE [DE-AC02-06CH11357]
  4. Division Of Chemistry
  5. Direct For Mathematical & Physical Scien [1346572] Funding Source: National Science Foundation

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The quasi-2D nickelate La4Ni3O8 (La-438), consisting of trilayer networks of square planar Ni ions, is a member of the so-called T' family, which is derived from the Ruddlesden-Popper (R-P) parent compound La4Ni3O10-x by removing two oxygen atoms and rearranging the rock salt layers to fluorite-type layers. Although previous studies on polycrystalline samples have identified a 105-K phase transition with a pronounced electronic and magnetic response but weak lattice character, no consensus on the origin of this transition has been reached. Here, we show using synchrotron X-ray diffraction on high-pO(2) floating zone-grown single crystals that this transition is associated with a real space ordering of charge into a quasi-2D charge stripe ground state. The charge stripe superlattice propagation vector, q = (2/3, 0, 1), corresponds with that found in the related 1/3-hole doped single- layer R-P nickelate, La5/3Sr1/3NiO4 (LSNO-1/3; Ni2.33+), with orientation at 45 degrees to the Ni-O bonds. The charge stripes in La-438 are weakly correlated along c to form a staggered ABAB stacking that reduces the Coulomb repulsion among the stripes. Surprisingly, however, we find that the charge stripes within each trilayer of La-438 are stacked in phase from one layer to the next, at odds with any simple Coulomb repulsion argument.

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