Location via proxy:   [ UP ]  
[Report a bug]   [Manage cookies]                

Suppression of the orbital magnetic moment driven by electronic correlations in Sr4Ru3O10

Filomena Forte, Lucia Capogna, Veronica Granata, Rosalba Fittipaldi, Antonio Vecchione, and Mario Cuoco
Phys. Rev. B 100, 104440 – Published 30 September 2019

Abstract

The coupling of spin and orbital degrees of freedom in the trilayer Sr4Ru3O10 sets a long-standing puzzle due to the peculiar anisotropic coexistence of out-of-plane ferromagnetism and in-plane metamagnetism. Recently, the induced magnetic structure by in-plane applied fields was investigated by means of spin-polarized neutron diffraction, which allowed the extraction of a substantial orbital component of the magnetic densities at Ru sites. It has been argued that the latter is at the origin of the evident layer-dependent magnetic anisotropy, where the inner layers carry larger magnetic momenta than the outer ones. We present a spin-polarized neutron diffraction study in order to characterize the nature of the ferromagnetic state of Sr4Ru3O10 in the presence of a magnetic field applied along the c axis. The components of the magnetic densities at the Ru sites reveal a vanishing contribution of the orbital magnetic moment which is unexpected for a material system where orbital and spin degeneracies are lifted by spin-orbit coupling and ferromagnetism. We employ a model that includes the Coulomb interaction and spin-orbit coupling at the Ru site to address the origin of the suppression of the orbital magnetic moment. The emerging scenario is that of nonlocal orbital degrees of freedom playing a significant role in the ferromagnetic phase, with a Coulomb interaction that is crucial to making an antialigned orbital moment at short distance, resulting in a ground state with vanishing local orbital moments.

  • Figure
  • Figure
  • Figure
  • Received 30 January 2019
  • Revised 31 July 2019

DOI:https://doi.org/10.1103/PhysRevB.100.104440

©2019 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Filomena Forte1,2,*, Lucia Capogna3, Veronica Granata1,2, Rosalba Fittipaldi1,2, Antonio Vecchione1,2, and Mario Cuoco1,2

  • 1Consiglio Nazionale delle Ricerche, SPIN, Via G. Paolo II 132, I-84084 Fisciano, Italy
  • 2Dipartimento di Fisica “E.R. Caianiello,” Università degli Studi di Salerno, Via G. Paolo II 132, I-84084 Fisciano, Italy
  • 3Consiglio Nazionale delle Ricerche, IOM OGG, and Institut Laue Langevin, 71 avenue des Martyrs, F-38042 Grenoble, France

  • *Corresponding author: filomena.forte@spin.cnr.it

Article Text (Subscription Required)

Click to Expand

References (Subscription Required)

Click to Expand
Issue

Vol. 100, Iss. 10 — 1 September 2019

Reuse & Permissions
Access Options
Author publication services for translation and copyediting assistance advertisement

Authorization Required


×

Images

  • Figure 1
    Figure 1

    Sections of the magnetization density in the ac plane of Sr4Ru3O10 calculated directly with the maximum entropy method. The two maps in the top panel are for a sample polarization in the ab plane, while the bottom ones correspond to a field applied along the c axis. In the color scale, magnetic density ranges from white (zero magnitude) to red (maximal value at Ruin for Bc). For quantitative estimates, refer to the values in Table 1.

    Reuse & Permissions
  • Figure 2
    Figure 2

    Evolution of (a) the spin and orbital components of the Ru magnetic density and (b) the Ru-Ru nonlocal orbital moment correlations projected along the c axis. B is the amplitude of the applied Zeeman field oriented along the c axis. We assume that t=0.4 eV, Δ1/t=0.3, Δ2/t=0.225, U/t=5.0, JH/U=0.2. AF-OM (CAF-OM) stands for a ferromagnetic ground state with antialigned orbital moments and inequivalent resulting orbital polarization with an averaged amplitude μavL=(1/2) (μ1L+μ2L) that is smaller (larger) than 0.1. B* indicates the amplitude of the Zeeman field above (below) which the ground state is spin polarized with a smaller (larger) averaged orbital moment than a given reference that is set at 0.1.

    Reuse & Permissions
  • Figure 3
    Figure 3

    Evolution of the AF-OM and CAF-OM ferromagnetic phases as a function of the c axis Zeeman field and of the octahedral distortions at the Ru1 site Δ1 for a given amplitude of the CF potential (elongated configuration) at Ru2. B is the amplitude of the applied magnetic field. We assume that t=0.4eV, Δ1/t=0.3, U/t=5.0, JH/U=0.2. AF-OM (CAF-OM) stands for a ground state with antialigned orbital moments and inequivalent resulting orbital polarization corresponding to an averaged amplitude μavL=(1/2) (μ1L+μ2L) that is smaller (larger) than 0.1. B* indicates the amplitude of the Zeeman field above (below) which the ground state is spin polarized with a smaller (larger) averaged orbital moment than a given reference that is set at 0.1.

    Reuse & Permissions
×

Sign up to receive regular email alerts from Physical Review B

Log In

Cancel
×

Search


Article Lookup

Paste a citation or DOI

Enter a citation
×