2004
DOI: 10.1103/physrevb.69.064426
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Bosonic representation of one-dimensional Heisenberg ferrimagnets

Abstract: We present a comparative study of bosonic languages to describe one-dimensional Heisenberg ferrimagnets. The ferrimagnetic Schwinger-boson mean-field theory demonstrated by Wu et al., the antiferromagnetic modified spin-wave theory designed by Takahashi, and its ferrimagnetic variant proposed by Yamamoto et al. are employed to calculate the energy structure and the thermodynamics of various ferrimagnets. A modified spin-wave scheme, which introduces a Lagrange multiplier keeping the native energy structure fre… Show more

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Cited by 49 publications
(58 citation statements)
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“…In the conventional spinwave scheme, the spin deviations in each sublattice diverge in the one-dimensional (1D) antiferromagnets, but the quantum as well as thermal divergence of the number of bosons can be overcome in the Takahashi scheme [17] that will be applied to the present antiferromagnetic F-F-AF chain. The AF-AF-F chain is a ferrimagnet, whose magnetization should be nonzero in the ground state but zero at finite temperature, leading to that we can apply the Yamamoto scheme [21,22], where the Lagrange multiplier was introduced directly in the free energy, to our present ferrimagnetic AF-AF-F chain. The detail derivations of the MSW formalism are collected in Appendix A, where the linear modified spin-wave (LMSW) theory, which is up to the order of O(S 1 ), and the perturbational interacting modified spin-wave (PIMSW) theory, which is up to the order of O(S 0 ), are included.…”
Section: Modified Spin-wave Theorymentioning
confidence: 99%
“…In the conventional spinwave scheme, the spin deviations in each sublattice diverge in the one-dimensional (1D) antiferromagnets, but the quantum as well as thermal divergence of the number of bosons can be overcome in the Takahashi scheme [17] that will be applied to the present antiferromagnetic F-F-AF chain. The AF-AF-F chain is a ferrimagnet, whose magnetization should be nonzero in the ground state but zero at finite temperature, leading to that we can apply the Yamamoto scheme [21,22], where the Lagrange multiplier was introduced directly in the free energy, to our present ferrimagnetic AF-AF-F chain. The detail derivations of the MSW formalism are collected in Appendix A, where the linear modified spin-wave (LMSW) theory, which is up to the order of O(S 1 ), and the perturbational interacting modified spin-wave (PIMSW) theory, which is up to the order of O(S 0 ), are included.…”
Section: Modified Spin-wave Theorymentioning
confidence: 99%
“…The quantum Hall ferrimagnetic states, or spin unbalanced phases, 24,25 are also a direct manifestation of coherent quantum mechanical tunneling and inter-dot electronic correlations. These states can be described in terms of linear combinations of spin excitons localized in left and right dots, which in turn lead to coherent spin oscillations, e.g., spin counterpart of coherent charge oscillations in H + 2 molecules.…”
Section: Introductionmentioning
confidence: 99%
“…(see Ref. [13]). α † k and β † k are the creation operators of the ferromagnetic and antiferromagnetic spin waves with momentum k, respectively.…”
Section: Modified Spin Wave Theorymentioning
confidence: 99%