<p>The Onsager Lie algebra <i>O</i> is an infinite-dimensional Lie algebra defined by generators <i>A</i> and <i>B</i> and relations <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\([A, [A, [A, B]]] = 4[A, B]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">[</mo> <mi>A</mi> <mo>,</mo> <mo stretchy="false">[</mo> <mi>A</mi> <mo>,</mo> <mo stretchy="false">[</mo> <mi>A</mi> <mo>,</mo> <mi>B</mi> <mo stretchy="false">]</mo> <mo stretchy="false">]</mo> <mo stretchy="false">]</mo> <mo>=</mo> <mn>4</mn> <mo stretchy="false">[</mo> <mi>A</mi> <mo>,</mo> <mi>B</mi> <mo stretchy="false">]</mo> </mrow> </math></EquationSource> </InlineEquation>, and <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\([B, [B, [B, A]]] = 4[B, A]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">[</mo> <mi>B</mi> <mo>,</mo> <mo stretchy="false">[</mo> <mi>B</mi> <mo>,</mo> <mo stretchy="false">[</mo> <mi>B</mi> <mo>,</mo> <mi>A</mi> <mo stretchy="false">]</mo> <mo stretchy="false">]</mo> <mo stretchy="false">]</mo> <mo>=</mo> <mn>4</mn> <mo stretchy="false">[</mo> <mi>B</mi> <mo>,</mo> <mi>A</mi> <mo stretchy="false">]</mo> </mrow> </math></EquationSource> </InlineEquation>. Using an embedding of <i>O</i> into the tetrahedron Lie algebra <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\boxtimes \)</EquationSource> <EquationSource Format="MATHML"><math> <mo>⊠</mo> </math></EquationSource> </InlineEquation>, we obtain four direct sum decompositions of the vector space <i>O</i>, each consisting of three summands. As we will show, there is a natural action of <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\mathbb {Z}_2 \times \mathbb {Z}_2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="double-struck">Z</mi> <mn>2</mn> </msub> <mo>×</mo> <msub> <mi mathvariant="double-struck">Z</mi> <mn>2</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> on these decompositions. For each decomposition, we provide a basis for each summand. Moreover, we describe the Lie bracket action on these bases and show how they are recursively constructed from the generators <i>A</i> and <i>B</i> of <i>O</i>. Finally, we discuss the action of <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\mathbb {Z}_2 \times \mathbb {Z}_2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="double-struck">Z</mi> <mn>2</mn> </msub> <mo>×</mo> <msub> <mi mathvariant="double-struck">Z</mi> <mn>2</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> on these bases and determine some transition matrices among the bases.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Four bases for the Onsager Lie algebra related by a \(\mathbb {Z}_2 \times \mathbb {Z}_2\) action

  • Jae-Ho Lee

摘要

The Onsager Lie algebra O is an infinite-dimensional Lie algebra defined by generators A and B and relations \([A, [A, [A, B]]] = 4[A, B]\) [ A , [ A , [ A , B ] ] ] = 4 [ A , B ] , and \([B, [B, [B, A]]] = 4[B, A]\) [ B , [ B , [ B , A ] ] ] = 4 [ B , A ] . Using an embedding of O into the tetrahedron Lie algebra \(\boxtimes \) , we obtain four direct sum decompositions of the vector space O, each consisting of three summands. As we will show, there is a natural action of \(\mathbb {Z}_2 \times \mathbb {Z}_2\) Z 2 × Z 2 on these decompositions. For each decomposition, we provide a basis for each summand. Moreover, we describe the Lie bracket action on these bases and show how they are recursively constructed from the generators A and B of O. Finally, we discuss the action of \(\mathbb {Z}_2 \times \mathbb {Z}_2\) Z 2 × Z 2 on these bases and determine some transition matrices among the bases.