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Applications of the Jordan and Lie algebras for some dynamical systems having internal symmetries - MaRDI portal

Applications of the Jordan and Lie algebras for some dynamical systems having internal symmetries (Q2761901)

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scientific article; zbMATH DE number 1686478
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Applications of the Jordan and Lie algebras for some dynamical systems having internal symmetries
scientific article; zbMATH DE number 1686478

    Statements

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    7 January 2002
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    dynamical systems
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    Jordan algebra
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    Lie algebra
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    Lie group
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    internal symmetry
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    Applications of the Jordan and Lie algebras for some dynamical systems having internal symmetries (English)
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    The author of this very interesting paper considers the applications of the Jordan and Lie algebras to some dynamical systems having internal symmetries. For the \(g\)-based Jordan algebra introduced by the author [Int. J. Non-linear Mech. 35, 421-429 (2000)] one assigns a matrix representation, which is proved to form a \(g\)-based Lie algebra under the commutator product. Then a new dynamical system based on the composition of the \(g\)-based Jordan and Lie algebras is derived. This dynamical system possesses the internal symmetry group \(\text{DSO}_0(n,1)\) and its projection \(\text{PDSO}_0(n,1)\). The author extends those results to the \(i\)-based formulations, of which the resulting dynamical system has internal symmetry group \(\text{DSO}(n+1)\), and its projection \(\text{PDSO}(n+1)\). The above underlying algebras are all nonassociative. However, for three-dimensional problems it is possible to add an extra term in the product to construct other algebras, which include two associative algebras, namely the \(i\)-based quaternion \(\mathbb{H}\) and the \(g\)- and \(i\)-based (mixed) quaternion \(\mathbb{H}_-^+\), and one noncommutative Jordan algebra. For the second case the author formulates a dynamical system with internal symmetry group \(\text{DSO}(2,2)\) and its projection \(\text{PDSO}(2,2)\), and also derives a rotation formula in the three-dimensional Minkowski space \(\mathbf M^3\). Several physical examples are given to illustrate this new formulation.
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