Condensed Matter Physics, 2020, vol. 23, No. 4, 43702
DOI:10.5488/CMP.23.43702
arXiv:2101.05164
Title:
Heisenberg spin chains with additional isotropic three-site exchange interactions
Author(s):
 
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N.B. Ivanov
(Institute of Solid State Physics, Bulgarian Academy of Sciences, Tzarigradsko chaussée 72, 1784 Sofia, Bulgaria)
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The J1-J3 Heisenberg spin models with nearest-neighbor (J1) and additional isotropic
three-site (J3) spin interactions remain relatively less explored, although such types of competing exchange terms
can naturally emerge from different sources, including the strong-coupling expansion of the multiorbital Hubbard model. Below we
present a short survey of the recently published research in this field, the emphasis being on the characteristics of the variety
of quantum phases supported by a few generic uniform- and alternating-spin J1-J3 Heisenberg chains.
For the reason that the positive (J3>0) three-site couplings tend towards the formation of local quantum dimers,
the J1-J3 spin models typically experience some spontaneous dimerization upon increasing J3.
Actually, it occurred that the established dimer phases in spin-S J1-J3 Heisenberg chains
(S>1/2) serve as complete analogues of the famous gapped Majumdar-Ghosh dimer phase in the spin-1/2 Heisenberg
chain with next-nearest-neighbor couplings. The same dimerizations have been observed in the alternating-spin (S,σ)
J1-J3 chains (S>σ), provided that the cell spin S+σ= integer, whereas for
half-integer cell spin, the local dimer formation produces gapless spin-liquid ground states. The alternating-spin
J1-J3 chains also provide some typical examples of spin models supporting the so-called non-Lieb-Mattis
magnetic phases.
Key words:
spin chains, quantum spin phases, three-spin interactions
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