Abstract <p>We prove the following assertion. Let <i>A</i> and <i>B</i> be nonsingular unitoids with simple canonical angles. Assume that their cosquares <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11470_2025_2189_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="TEX">\({{\mathcal{C}}_{A}}\)</EquationSource> <!--ComMat2470208Ikramov-m1--> </InlineEquation> = <i>A</i><sup>–</sup>*<i>A</i> and <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11470_2025_2189_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="TEX">\({{\mathcal{C}}_{B}}\)</EquationSource> <!--ComMat2470208Ikramov-m2--> </InlineEquation> = <i>B</i><sup>–</sup>*<i>B</i> commute. Bring both cosquares to diagonal form by one and the same similarity (simultaneous diagonalization). The resulting diagonal matrices Λ and <i>M</i> have unimodular diagonal entries. Denote by <i>D</i><sub><i>A</i></sub> and <i>D</i><sub><i>B</i></sub> a pair of diagonal matrices whose cosquares are Λ and <i>M</i>, respectively. The congruence orbits generated by <i>D</i><sub><i>A</i></sub> and <i>D</i><sub><i>B</i></sub> will be denoted by <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11470_2025_2189_Article_IEq3.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="51" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal{O}({{D}_{A}})\)</EquationSource> <!--ComMat2470208Ikramov-m3--> </InlineEquation> and <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11470_2025_2189_Article_IEq4.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="52" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal{O}({{D}_{B}})\)</EquationSource> <!--ComMat2470208Ikramov-m4--> </InlineEquation>. Let <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11470_2025_2189_Article_IEq5.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(\tilde {A}\)</EquationSource> <!--ComMat2470208Ikramov-m5--> </InlineEquation> and <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11470_2025_2189_Article_IEq6.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(\tilde {B}\)</EquationSource> <!--ComMat2470208Ikramov-m6--> </InlineEquation> be the points of these orbits corresponding to the same transition matrix <i>P</i>, that is, <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11470_2025_2189_Article_IEq7.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(\tilde {A}\)</EquationSource> <!--ComMat2470208Ikramov-m7--> </InlineEquation> = <i>P</i>*<i>D</i><sub><i>A</i></sub><i>P</i>, <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11470_2025_2189_Article_IEq8.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(\tilde {B}\)</EquationSource> <!--ComMat2470208Ikramov-m8--> </InlineEquation> = <i>P</i>*<i>D</i><sub><i>B</i></sub><i>P</i>. Then <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11470_2025_2189_Article_IEq9.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(\tilde {A}\)</EquationSource> <!--ComMat2470208Ikramov-m9--> </InlineEquation> and <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11470_2025_2189_Article_IEq10.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(\tilde {B}\)</EquationSource> <!--ComMat2470208Ikramov-m10--> </InlineEquation> satisfy the relations <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11470_2025_2189_Article_IEq11.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="46" /> </InlineMediaObject> <EquationSource Format="TEX">\(\tilde {A}{{\tilde {B}}^{ - }}\text{*}\)</EquationSource> <!--ComMat2470208Ikramov-m11--> </InlineEquation> = <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11470_2025_2189_Article_IEq12.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="46" /> </InlineMediaObject> <EquationSource Format="TEX">\(\tilde {B}{{\tilde {A}}^{ - }}\text{*}\)</EquationSource> <!--ComMat2470208Ikramov-m12--> </InlineEquation> and <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11470_2025_2189_Article_IEq13.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="49" /> </InlineMediaObject> <EquationSource Format="TEX">\({{\tilde {A}}^{ - }}\text{*}{\kern 1pt} \tilde {B}\)</EquationSource> <!--ComMat2470208Ikramov-m13--> </InlineEquation> = <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11470_2025_2189_Article_IEq14.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="50" /> </InlineMediaObject> <EquationSource Format="TEX">\({{\tilde {B}}^{ - }}\text{*}{\kern 1pt} \tilde {A}\)</EquationSource> <!--ComMat2470208Ikramov-m14--> </InlineEquation>. In theory of congruences, these relations can be regarded as a kind of substitute for the conventional permutability.</p>

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Simultaneous Diagonalization of Two Matrices: Simularities and Congruences

  • Kh. D. Ikramov,
  • A. M. Nazari

摘要

Abstract

We prove the following assertion. Let A and B be nonsingular unitoids with simple canonical angles. Assume that their cosquares \({{\mathcal{C}}_{A}}\) = A*A and \({{\mathcal{C}}_{B}}\) = B*B commute. Bring both cosquares to diagonal form by one and the same similarity (simultaneous diagonalization). The resulting diagonal matrices Λ and M have unimodular diagonal entries. Denote by DA and DB a pair of diagonal matrices whose cosquares are Λ and M, respectively. The congruence orbits generated by DA and DB will be denoted by \(\mathcal{O}({{D}_{A}})\) and \(\mathcal{O}({{D}_{B}})\) . Let \(\tilde {A}\) and \(\tilde {B}\) be the points of these orbits corresponding to the same transition matrix P, that is, \(\tilde {A}\) = P*DAP, \(\tilde {B}\) = P*DBP. Then \(\tilde {A}\) and \(\tilde {B}\) satisfy the relations \(\tilde {A}{{\tilde {B}}^{ - }}\text{*}\) = \(\tilde {B}{{\tilde {A}}^{ - }}\text{*}\) and \({{\tilde {A}}^{ - }}\text{*}{\kern 1pt} \tilde {B}\) = \({{\tilde {B}}^{ - }}\text{*}{\kern 1pt} \tilde {A}\) . In theory of congruences, these relations can be regarded as a kind of substitute for the conventional permutability.