<p>In the general setting of the adjointable operators on Hilbert <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43037_2025_444_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="TEX">\(C^*\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>C</mi> <mo>∗</mo> </msup> </math></EquationSource> </InlineEquation>-modules, this paper deals mainly with the weighted Moore–Penrose inverse (briefly weighted M–P inverse) <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43037_2025_444_Article_IEq2.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="38" /> </InlineMediaObject> <EquationSource Format="TEX">\(A^\dag _{MN}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>A</mi> <mrow> <mi mathvariant="italic">MN</mi> </mrow> <mo>†</mo> </msubsup> </math></EquationSource> </InlineEquation> in the case that the weights <i>M</i> and <i>N</i> are self-adjoint invertible operators, which need not to be positive. A new formula linking <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43037_2025_444_Article_IEq2.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="38" /> </InlineMediaObject> <EquationSource Format="TEX">\(A^\dag _{MN}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>A</mi> <mrow> <mi mathvariant="italic">MN</mi> </mrow> <mo>†</mo> </msubsup> </math></EquationSource> </InlineEquation> to <i>A</i>, <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43037_2025_444_Article_IEq4.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="TEX">\(A^\dag \)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>A</mi> <mo>†</mo> </msup> </math></EquationSource> </InlineEquation>, <i>M</i> and <i>N</i> is derived, in which <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43037_2025_444_Article_IEq4.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="TEX">\(A^\dag \)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>A</mi> <mo>†</mo> </msup> </math></EquationSource> </InlineEquation> denotes the M–P inverse of <i>A</i>. Based on this formula, some new results on the weighted M–P inverse are obtained. Firstly, it is shown that <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43037_2025_444_Article_IEq6.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="89" /> </InlineMediaObject> <EquationSource Format="TEX">\(A^\dag _{MN}=A^\dag _{ST}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>A</mi> <mrow> <mi mathvariant="italic">MN</mi> </mrow> <mo>†</mo> </msubsup> <mo>=</mo> <msubsup> <mi>A</mi> <mrow> <mi mathvariant="italic">ST</mi> </mrow> <mo>†</mo> </msubsup> </mrow> </math></EquationSource> </InlineEquation> for some positive definite operators <i>S</i> and <i>T</i>. This shows that <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43037_2025_444_Article_IEq2.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="38" /> </InlineMediaObject> <EquationSource Format="TEX">\(A^\dag _{MN}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>A</mi> <mrow> <mi mathvariant="italic">MN</mi> </mrow> <mo>†</mo> </msubsup> </math></EquationSource> </InlineEquation> is essentially an ordinary weighted M–P inverse. Secondly, some limit formulas for the ordinary weighted M–P inverse originally known for matrices are generalized and improved. Thirdly, it is shown that when <i>A</i>,&#xa0;<i>M</i> and <i>N</i> act on the same Hilbert <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43037_2025_444_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="TEX">\(C^*\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>C</mi> <mo>∗</mo> </msup> </math></EquationSource> </InlineEquation>-module, <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43037_2025_444_Article_IEq2.gif" Format="GIF" Height="23" Rendition="HTML" Resolution="72" Type="Linedraw" Width="38" /> </InlineMediaObject> <EquationSource Format="TEX">\(A^\dag _{MN}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>A</mi> <mrow> <mi mathvariant="italic">MN</mi> </mrow> <mo>†</mo> </msubsup> </math></EquationSource> </InlineEquation> belongs to the <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43037_2025_444_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="22" /> </InlineMediaObject> <EquationSource Format="TEX">\(C^*\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>C</mi> <mo>∗</mo> </msup> </math></EquationSource> </InlineEquation>-algebra generated by <i>A</i>, <i>M</i> and <i>N</i>. Finally, some characterizations of the continuity of the weighted M–P inverse are provided.</p>

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A new formula for the weighted Moore–Penrose inverse and its applications

  • Qingxiang Xu

摘要

In the general setting of the adjointable operators on Hilbert \(C^*\) C -modules, this paper deals mainly with the weighted Moore–Penrose inverse (briefly weighted M–P inverse) \(A^\dag _{MN}\) A MN in the case that the weights M and N are self-adjoint invertible operators, which need not to be positive. A new formula linking \(A^\dag _{MN}\) A MN to A, \(A^\dag \) A , M and N is derived, in which \(A^\dag \) A denotes the M–P inverse of A. Based on this formula, some new results on the weighted M–P inverse are obtained. Firstly, it is shown that \(A^\dag _{MN}=A^\dag _{ST}\) A MN = A ST for some positive definite operators S and T. This shows that \(A^\dag _{MN}\) A MN is essentially an ordinary weighted M–P inverse. Secondly, some limit formulas for the ordinary weighted M–P inverse originally known for matrices are generalized and improved. Thirdly, it is shown that when AM and N act on the same Hilbert \(C^*\) C -module, \(A^\dag _{MN}\) A MN belongs to the \(C^*\) C -algebra generated by A, M and N. Finally, some characterizations of the continuity of the weighted M–P inverse are provided.