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Diversity of quantum ground states and quantum phase transitions of a spin-12 Heisenberg octahedral chain

Jozef Strečka, Johannes Richter, Oleg Derzhko, Taras Verkholyak, and Katarína Karľová
Phys. Rev. B 95, 224415 – Published 13 June 2017

Abstract

The spin-12 Heisenberg octahedral chain with regularly alternating monomeric and square-plaquette sites is investigated using various analytical and numerical methods: variational technique, localized-magnon approach, exact diagonalization (ED), and density-matrix renormalization group (DMRG) methods. The model belongs to the class of flatband systems and it has a rich ground-state phase diagram including phases with spontaneously broken translational symmetry. Moreover, it exhibits an anomalous low-temperature thermodynamics close to continuous or discontinuous field-driven quantum phase transitions between three quantum ferrimagnetic phases, tetramer-hexamer phase, monomer-tetramer phase, localized-magnon phase, and two different spin-liquid phases. If the intraplaquette coupling is at least twice as strong as the monomer-plaquette coupling, the variational method furnishes a rigorous proof of the monomer-tetramer ground state in a low-field region and the localized-magnon approach provides exact evidence of a single magnon trapped at each square plaquette in a high-field region. In the rest of the parameter space we have numerically studied the ground-state phase diagram and magnetization process using DMRG and ED methods. It is shown that the zero-temperature magnetization curve may involve up to four intermediate plateaus at zero, one-fifth, two-fifths, and three-fifths of the saturation magnetization, while the specific heat exhibits a striking low-temperature peak in the vicinity of discontinuous quantum phase transitions.

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  • Received 2 March 2017
  • Revised 19 April 2017

DOI:https://doi.org/10.1103/PhysRevB.95.224415

©2017 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Jozef Strečka1,*, Johannes Richter2, Oleg Derzhko3,4, Taras Verkholyak3, and Katarína Karľová1

  • 1Institute of Physics, Faculty of Science, P. J. Šafárik University, Park Angelinum 9, 04001 Košice, Slovakia
  • 2Institut für Theoretische Physik, Otto-von-Guericke Universität in Magdeburg, 39016 Magdeburg, Germany
  • 3Institute for Condensed Matter Physics, NASU, Svientsitskii Street 1, 79011 L'viv, Ukraine
  • 4Department for Theoretical Physics, Ivan Franko National University of L'viv, Drahomanov Street 12, 79005 L'viv, Ukraine

  • *jozef.strecka@upjs.sk

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Vol. 95, Iss. 22 — 1 June 2017

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Images

  • Figure 1
    Figure 1

    A diagrammatic representation of the spin-12 Heisenberg octahedral chain. Thick (blue) lines represent the Heisenberg intraplaquette coupling J2, while thin (red) lines correspond to the monomer-plaquette coupling J1.

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  • Figure 2
    Figure 2

    The unit cell of the spin-12 Heisenberg octahedral chain, which is constituted by a five-spin cluster with the geometric shape of a square pyramid.

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  • Figure 3
    Figure 3

    The one-magnon energy bands (11) of the spin-12 Heisenberg octahedral chain for four different values of the interaction ratio: (a) J2/J1=1, (b) J2/J1=2, (c) J2/J1=3, and (d) J2/J1=4.

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  • Figure 4
    Figure 4

    A schematic representation of the singlet tetramer-hexamer state (27). Thick (black) ovals represent singlet states of tetramers and hexamers given by Eqs. (6) and (28), respectively.

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  • Figure 5
    Figure 5

    The zero-field ground-state phase diagram of the spin-12 Heisenberg octahedral chain. The numbers in square brackets determine within a given ground state the total spin on monomeric sites and square plaquettes. Note that the ferrimagnetic phase (1/2-2-1/2-1) and the monomer-tetramer phase (1/2-1-1/2-0) break the translational symmetry.

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  • Figure 6
    Figure 6

    The ground-state phase diagram of the spin-12 Heisenberg octahedral chain in the J2/J1h/J1 plane. A thick line schematically shows the quantum ferrimagnetic ground state, which originates from the effective mixed spin-(12,2,12,1) Heisenberg chain and is stable in a very narrow interval of the magnetic fields.

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  • Figure 7
    Figure 7

    A few typical zero-temperature magnetization curves of the spin-12 Heisenberg octahedral chain. Thick solid lines show numerical results based on DMRG calculations for the finite-size chain of L=300 spins (N=60 unit cells) and thin broken lines illustrate numerical ED results for the finite-size chain of L=40 spins (N=8 unit cells) by assuming six different values of the interaction ratio: (a) J2/J1=0.5, (b) J2/J1=0.7, (c) J2/J1=1.2, (d) J2/J1=1.6, (e) J2/J1=1.8, and (f) J2/J1=2.0.

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  • Figure 8
    Figure 8

    The magnetization (upper panel) and specific heat (lower panel) of the spin-12 Heisenberg octahedral chain as a function of the magnetic field and temperature for the fixed value of the interaction ratio J2/J1=3. Solid lines follow from Eqs. (16) and (17) derived by means of the localized-magnon approach, while broken lines of different styles illustrate the full ED data for the finite-size chain of L=20 spins (N=4 unit cells).

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