2007
DOI: 10.1002/pssb.200674624
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An explicit demonstration of integrability for the linear Heisenberg chain of N = 9 nodes

Abstract: We propose the system of 1 8 N -= mutually commuting operators which classify all eigenstates of the Heisenberg Hamiltonian for the linear magnetic chain of N = 9 nodes, each with the spin 1/2. These eigenstates, determined exactly by Bethe Ansatz and classified combinatorially by rigged string configurations of Kerov, Kirillov and Reshetikhin, can be also associated with the spectrum of this set of commuting operators.

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Cited by 3 publications
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“…We use the algebraic Bethe ansatz approach of Faddeev and Takhtajan [9,10] to derive explicitly the set of N − 1 mutually commuting operators (involving the Heisenberg Hamiltonian for the XXX model) from the corresponding monodromy matrix, point out some their general properties and special cases, and compare on some examples the resulting eigenstates with the exact Bethe ansatz solutions, classified by rigged string configurations, as defined by Kerov, Kirillov and Reshetikhin [7]. Some preliminary results on these operators have been reported in our previous papers [11,12].…”
Section: Introductionmentioning
confidence: 99%
“…We use the algebraic Bethe ansatz approach of Faddeev and Takhtajan [9,10] to derive explicitly the set of N − 1 mutually commuting operators (involving the Heisenberg Hamiltonian for the XXX model) from the corresponding monodromy matrix, point out some their general properties and special cases, and compare on some examples the resulting eigenstates with the exact Bethe ansatz solutions, classified by rigged string configurations, as defined by Kerov, Kirillov and Reshetikhin [7]. Some preliminary results on these operators have been reported in our previous papers [11,12].…”
Section: Introductionmentioning
confidence: 99%