<p>Let <i>V</i> be a unitary vector space. Suppose <i>H</i> is a subgroup of the symmetric group <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(S_m\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>S</mi> <mi>m</mi> </msub> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\Lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Λ</mi> </math></EquationSource> </InlineEquation> an irreducible unitary representation of <i>H</i> over a unitary space <i>U</i>. Denote by <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(V_{\Lambda }(H)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>V</mi> <mi mathvariant="normal">Λ</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>H</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> the generalized symmetry class of tensors over <i>V</i> associated with <i>H</i> and <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\Lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Λ</mi> </math></EquationSource> </InlineEquation>. In this paper, we show that the vector space <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(V_{\Lambda }(H)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>V</mi> <mi mathvariant="normal">Λ</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>H</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> has always an orthogonal basis consisting generalized decomposable symmetrized tensors. By determining the group module structure of generalized coset spaces, we give a group module structure for generalized orbital subspaces.</p>

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Orthogonal basis and group module structure for generalized symmetry classes of tensors

  • Yousef Zamani,
  • Rasoul Khalilzadeh

摘要

Let V be a unitary vector space. Suppose H is a subgroup of the symmetric group \(S_m\) S m and \(\Lambda \) Λ an irreducible unitary representation of H over a unitary space U. Denote by \(V_{\Lambda }(H)\) V Λ ( H ) the generalized symmetry class of tensors over V associated with H and \(\Lambda \) Λ . In this paper, we show that the vector space \(V_{\Lambda }(H)\) V Λ ( H ) has always an orthogonal basis consisting generalized decomposable symmetrized tensors. By determining the group module structure of generalized coset spaces, we give a group module structure for generalized orbital subspaces.