2004
DOI: 10.1353/ajm.2004.0035
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The Lagrange bitop on so (4) × so (4) and geometry of the Prym varieties

Abstract: Abstract. A four-dimensional integrable rigid-body system is considered and it is shown that it represents two twisted three-dimensional Lagrange tops. A polynomial Lax representation, which doesn't fit neither in Dubrovin's nor in Adler-van Moerbeke's picture is presented. The algebro-geometric integration procedure is based on deep facts from the geometry of the Prym varieties of double coverings of hyperelliptic curves. The correspondence between all such coverings with Prym varieties splitted as a sum of t… Show more

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Cited by 10 publications
(69 citation statements)
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“…is the Hamiltonian function of the Lagrange bitop. The Lagrange bitop is a complete integrable system of a heavy rigid body on so(4) × so(4) defined in [18] and studied in details in [19]. Moreover, the Lagrange bitop is a bi-Hamiltonian system.…”
Section: 2mentioning
confidence: 99%
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“…is the Hamiltonian function of the Lagrange bitop. The Lagrange bitop is a complete integrable system of a heavy rigid body on so(4) × so(4) defined in [18] and studied in details in [19]. Moreover, the Lagrange bitop is a bi-Hamiltonian system.…”
Section: 2mentioning
confidence: 99%
“…In other words, the systems (7.10), restricted to (7.14), is an example of integrable isoholomorhic system ( [19], see Remark 8.2 given below).…”
Section: Partial Reduction Of Rigid Body Systemsmentioning
confidence: 99%
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