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Superconductivity in infinite-layer nickelates: Role of f orbitals

Subhadeep Bandyopadhyay, Priyo Adhikary, Tanmoy Das, Indra Dasgupta, and Tanusri Saha-Dasgupta
Phys. Rev. B 102, 220502(R) – Published 10 December 2020

Abstract

Employing first-principles density functional theory calculations and Wannierization of the low-energy band structure, we analyze the electronic structure of undoped, infinite-layer nickelate compounds NdNiO2, PrNiO2, and LaNiO2. Our study reveals the important role of the nonzero f-ness of Nd and Pr atoms, as opposed to the f0 occupancy of La. The nonzero f-ness becomes effective in lowering the energy of the rare-earth 5d hybridized axial orbital, thereby enhancing the electron pockets and influencing the Fermi surface topology. The Fermi surface topology of NdNiO2 and PrNiO2 is strikingly similar, while differences are observed for LaNiO2. This difference shows up in computed doping-dependent superconducting properties of the three compounds within a weak coupling theory, which finds two-gap superconductivity for NdNiO2 and PrNiO2, and the possibility of a single-gap superconductivity for LaNiO2 with the strength of superconductivity suppressed by almost a factor of 2, compared to the Nd or Pr compound.

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  • Received 28 September 2020
  • Revised 17 November 2020
  • Accepted 17 November 2020

DOI:https://doi.org/10.1103/PhysRevB.102.220502

©2020 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Subhadeep Bandyopadhyay1,*, Priyo Adhikary2,*, Tanmoy Das2,†, Indra Dasgupta1,‡, and Tanusri Saha-Dasgupta3,§

  • 1School of Physical Sciences, Indian Association for the Cultivation of Science, Kolkata 700 032, India
  • 2Department of Physics, Indian Institute of Science, Bangalore 560012, India
  • 3S. N. Bose National Centre for Basic Sciences, JD Block, Sector III, Salt Lake, Kolkata, West Bengal 700106, India

  • *These authors contributed equally to this work.
  • tnmydas@gmail.com
  • sspid@iacs.res.in
  • §t.sahadasgupta@gmail.com

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Issue

Vol. 102, Iss. 22 — 1 December 2020

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Images

  • Figure 1
    Figure 1

    (a) Crystal structure of infinite-layer RNiO2 (R=Pr/Nd/La). (b) DFT band structure of LaNiO2 (black, solid lines) in comparison to NdNiO2 (red, dashed lines) and PrNiO2 (blue, dashed lines) plotted along the high-symmetry lines [Γ(0,0,0)X(π/a,0,0)M(π/a,π/a,0)ΓZ(0,0,π/c)R(π/a,0,π/c)A(π/a,π/a,π/c)] of the tetragonal Brillouin zone, computed for the actual crystals of LaNiO2, NdNiO2, and PrNiO2. (c) Same as (b) but band structures computed using the same crystal structure (crystal structure of LaNiO2) for all three compounds. The zero of the energy is set to the Fermi level. (d)–(f) The density of states corresponding to the two-band crossing Fermi level for (d) LaNiO2, (e) PrNiO2, and (f) NdNiO2. Labeled are the occupancies of the two bands. (g)–(i) The Fermi surfaces for (g) LaNiO2, (h) PrNiO2, and (i) NdNiO2.

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  • Figure 2
    Figure 2

    (a)–(c) The effective Ni x2y2 Wannier function for (a) LaNiO2, (b) PrNiO2, and (c) NdNiO2. The oppositely signed lobes are colored differently. (d)–(f) The effective axial Wannier function for (d) LaNiO2, (e) PrNiO2, and (f) NdNiO2. (g)–(i) The in-plane and out-of-plane (insets) intra- and interorbital hopping interactions plotted as a function of Ni-Ni distances: between (g) axial-axial, (h) x2y2x2y2, and (i) x2y2-axial. The distances corresponding to various near neighbors (NNs) are marked. The interactions for LaNiO2, PrNiO2, and NdNiO2 are shown as circles, triangles, and squares.

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  • Figure 3
    Figure 3

    (a) Doping-dependent SC coupling constant λ (scaled by the strength of maximum λ for NNO) for three different materials for a choice of V=1.5eV and V=1.0eV. The shaded regions are a guide to the eyes. Due to the limitations of the weak coupling theory, the shaded areas for x<0.15 are only a schematic construction. (b) and (c) FS for NNO at two dopings, with the blue to red color map denoting the corresponding orbital weight for the Ni-dx2y2 to axial-s orbitals.

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