2009
DOI: 10.1016/j.nuclphysb.2009.04.024
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The Bethe ansatz equations for reflecting magnons

Abstract: We derive the Bethe ansatz equations on the half line for particles interacting through factorized S-matrices invariant relative to the centrally extended su(2|2) Lie superalgebra and su(1|2) open boundaries. These equations may be of relevance for the study of the spectrum of open strings on AdS 5 × S 5 background attached to Y = 0 giant graviton branes. A one-dimensional spin chain Hamiltonian associated to this system is also derived.

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Cited by 23 publications
(36 citation statements)
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“…Our ansatz of the eigenvalues of the transfer matrices passed through some consistency checks and should be compared with the all-loop asymptotic Bethe ansatz equations which need to be proposed. Such all-loop Bethe ansatz equations for N = 4 SYM were obtained in [22]. We have shown in [1] and this paper that determinant like operators provide integrable boundary conditions for the open spin chain in ABJM theory at least at planar two-loop level.…”
Section: Resultsmentioning
confidence: 60%
“…Our ansatz of the eigenvalues of the transfer matrices passed through some consistency checks and should be compared with the all-loop asymptotic Bethe ansatz equations which need to be proposed. Such all-loop Bethe ansatz equations for N = 4 SYM were obtained in [22]. We have shown in [1] and this paper that determinant like operators provide integrable boundary conditions for the open spin chain in ABJM theory at least at planar two-loop level.…”
Section: Resultsmentioning
confidence: 60%
“…Multiparticle states of the open string correspond to so-called determinant-like operators in the dual gauge theory. The Y − Y system, consisting of Y = 0 branes [10] at both ends of the string, was studied in [11,12,13]. The integrability of this model was exploited in [12,13] to compute wrapping corrections of one-particle states.…”
Section: Introductionmentioning
confidence: 99%
“…The detailed results depend on the specific boundary conditions at the two ends of the interval. Among the integrable cases that have been studied are Y = 0 branes [11,12] at both ends [13,14,15]; and Y = 0 at one end and Y = 0 at the other end [16]. (For a review of integrable boundary conditions in AdS/CFT, see [17].…”
Section: Introductionmentioning
confidence: 99%