1996
DOI: 10.1088/0305-4470/29/14/021
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Integrable spin chain with reflecting end

Abstract: A new integrable spin chain of the Haldane-Shastry type is introduced. It is interpreted as the inverse-square interacting spin chain with a reflecting end. The lattice points of this model consist of the square roots of the zeros of the Laguerre polynomial. Using the "exchange operator formalism", the integrals of motion for the model are explicitly constructed.

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Cited by 40 publications
(58 citation statements)
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“…As mentioned above, this problem is equivalent to the triangularization of the extensionsH andH sc acting on their respective Hilbert spaces H ≡ Λ εε (L 2 (C (B) ) ⊗ Σ) and H sc ≡ Λ sc (L 2 (C (B) )), which can be carried out without difficulty with the help of Eq. (39).…”
Section: Triangularization Of H (B) and H (B)mentioning
confidence: 99%
See 1 more Smart Citation
“…As mentioned above, this problem is equivalent to the triangularization of the extensionsH andH sc acting on their respective Hilbert spaces H ≡ Λ εε (L 2 (C (B) ) ⊗ Σ) and H sc ≡ Λ sc (L 2 (C (B) )), which can be carried out without difficulty with the help of Eq. (39).…”
Section: Triangularization Of H (B) and H (B)mentioning
confidence: 99%
“…Spin generalizations of the BC N Calogero-Sutherland model have been extensively studied in the last few years, and various properties of their related spin chains of HS type have been analyzed with the help of the freezing trick [37][38][39][40][41][42][43][44]. Among the other classical root systems, the exceptional ones are comparatively less interesting in this context, since their associated models consist of at most 8 particles.…”
Section: Introductionmentioning
confidence: 99%
“…They are all associated with the root system A N−1 , in the sense that the interactions J i j depend only on the differences of the site coordinates ξ k . Although several generalizations of these chains to the BC N and D N root systems have been considered in the literature [7][8][9][10][11], in this paper we shall restrict ourselves to the above A N−1 -type models. Spin chains of HS type are the simplest models in condensed matter physics exhibiting fractional statistics [12].…”
Section: Introductionmentioning
confidence: 99%
“…Indeed, Olshanetsky and Perelomov established the existence of an underlying A N root system structure for both the spinless Calogero and Sutherland models, and constructed generalizations thereof associated with any (extended) root system [4]. Spin generalizations of the BC N Calogero and Sutherland models have also been proposed, and various properties of the related lattice models of HS type have been studied with the help of the freezing trick [38][39][40][41][42][43]. Among the other classical root systems, the exceptional ones are comparatively less interesting, since their associated models consist of at most 8 particles.…”
Section: Introductionmentioning
confidence: 99%