<p>We study a novel <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(n(n+1)/2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo stretchy="false">(</mo> <mi>n</mi> <mo>+</mo> <mn>1</mn> <mo stretchy="false">)</mo> <mo stretchy="false">/</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>-dimensional non-semisimple Lie algebra <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\mathfrak {g}_n\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="fraktur">g</mi> <mi>n</mi> </msub> </math></EquationSource> </InlineEquation>, a generalisation of both <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\mathfrak {sl}_2(\mathbb {K})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="fraktur">sl</mi> <mn>2</mn> </msub> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="double-struck">K</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> and the two-photon Lie algebra <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\mathfrak {h}_6\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="fraktur">h</mi> <mn>6</mn> </msub> </math></EquationSource> </InlineEquation>. We investigate its properties, including its structure, representations, and its Casimir elements. In particular, we prove that there exists only one non-trivial Casimir polynomial of degree <i>n</i> given by the determinant of an <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(n\times n\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>×</mo> <mi>n</mi> </mrow> </math></EquationSource> </InlineEquation> symmetric matrix. We then associate this Lie algebra to a hierarchy of Hamiltonian systems with integrability properties depending on <i>n</i> and describe their first integrals as sums of squares of linear combinations of the components of the angular momentum. In particular, we obtain that these systems are integrable for <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(n=2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>=</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>, quasi-integrable for <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(n=3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>=</mo> <mn>3</mn> </mrow> </math></EquationSource> </InlineEquation>, and of Poincaré–Lyapunov–Nekhoroshev type for <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(n\ge 4\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>≥</mo> <mn>4</mn> </mrow> </math></EquationSource> </InlineEquation>.</p>

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A Novel Chain of Lie Algebras and its Coalgebra Symmetry

  • Giorgio Gubbiotti,
  • Danilo Latini,
  • Bert van Geemen

摘要

We study a novel \(n(n+1)/2\) n ( n + 1 ) / 2 -dimensional non-semisimple Lie algebra \(\mathfrak {g}_n\) g n , a generalisation of both \(\mathfrak {sl}_2(\mathbb {K})\) sl 2 ( K ) and the two-photon Lie algebra \(\mathfrak {h}_6\) h 6 . We investigate its properties, including its structure, representations, and its Casimir elements. In particular, we prove that there exists only one non-trivial Casimir polynomial of degree n given by the determinant of an \(n\times n\) n × n symmetric matrix. We then associate this Lie algebra to a hierarchy of Hamiltonian systems with integrability properties depending on n and describe their first integrals as sums of squares of linear combinations of the components of the angular momentum. In particular, we obtain that these systems are integrable for \(n=2\) n = 2 , quasi-integrable for \(n=3\) n = 3 , and of Poincaré–Lyapunov–Nekhoroshev type for \(n\ge 4\) n 4 .