1998
DOI: 10.1103/physrevb.58.3117
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Elementary excitations in dimerized and frustrated Heisenberg chains

Abstract: We present a detailed numerical analysis of the low energy excitation spectrum of a frustrated and dimerized spin S = 1/2 Heisenberg chain. In particular, we show that in the commensurate spin-Peierls phase the ratio of the singlet and triplet excitation gap is a universal function which depends on the frustration parameter only. We identify the conditions for which a second elementary triplet branch in the excitation spectrum splits from the continuum. We compare our results with predictions from the continuu… Show more

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Cited by 90 publications
(130 citation statements)
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“…This behavior can be well compared to the singlet bound state observed in CuGeO 3 37 . The small binding energy of this signal just below 2 01 = 5 0 c m ;1 would only be expected for a singlet bound state in a spin chain with negligible frustration 8 . The weak spin-orbit coupling evidenced in ESR experiments 26 in addition excludes one-magnon scattering, e.g., from the upper dispersing branch ( 0 01 ) 17 in a direction.…”
Section: Quasielastic Scatteringmentioning
confidence: 99%
“…This behavior can be well compared to the singlet bound state observed in CuGeO 3 37 . The small binding energy of this signal just below 2 01 = 5 0 c m ;1 would only be expected for a singlet bound state in a spin chain with negligible frustration 8 . The weak spin-orbit coupling evidenced in ESR experiments 26 in addition excludes one-magnon scattering, e.g., from the upper dispersing branch ( 0 01 ) 17 in a direction.…”
Section: Quasielastic Scatteringmentioning
confidence: 99%
“…In the dimerized phase (purely magnetic 1D model) the excitations can be considered as local triplet and a corresponding two-particle continuum of triplet excitations. If a frustration of the spin system due to NNN intrachain exchange or an interchain interaction is taken into account, well-defined magnetic bound states also develop [33][34][35].…”
Section: Magnetic Raman Scatteringmentioning
confidence: 99%
“…We introduce the parameter α = J2 |J1| for convenience. This model with NN and NNN antiferromagnetic interactions (J 1 , J 2 > 0) is well studied [1][2][3][4][5][6][7][8] . This chain is well known to display a quantum phase transition from a gapless, translationally invariant state with algebraic spin correlations (the spin fluid phase) to dimer gapful state at α c ≃ 0.2411 3 .…”
Section: Introductionmentioning
confidence: 99%