Abstract <p>The concept of the weighted <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11957_2025_7227_Article_IEq5.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal{A}\)</EquationSource> <!--ContMath2460190Altwaijry-m5--> </InlineEquation>-numerical radius was recently defined, where <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11957_2025_7227_Article_IEq5.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal{A}\)</EquationSource> <!--ContMath2460190Altwaijry-m6--> </InlineEquation> is assumed to be a positive operator. In this paper, we introduce another weighted <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11957_2025_7227_Article_IEq5.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal{A}\)</EquationSource> <!--ContMath2460190Altwaijry-m7--> </InlineEquation>-numerical radius, denoted by <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11957_2025_7227_Article_IEq8.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="60" /> </InlineMediaObject> <EquationSource Format="TEX">\(\omega_{(\varepsilon,\mathcal{A})}\left(\cdot\right)\)</EquationSource> <!--ContMath2460190Altwaijry-m8--> </InlineEquation>, for operators in semi-Hilbert spaces. We establish some basic properties and inequalities for <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11957_2025_7227_Article_IEq8.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="60" /> </InlineMediaObject> <EquationSource Format="TEX">\(\omega_{(\varepsilon,\mathcal{A})}\left(\cdot\right)\)</EquationSource> <!--ContMath2460190Altwaijry-m9--> </InlineEquation>, which generalize earlier results about <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11957_2025_7227_Article_IEq10.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="39" /> </InlineMediaObject> <EquationSource Format="TEX">\(\omega_{\mathcal{A}}(\cdot)\)</EquationSource> <!--ContMath2460190Altwaijry-m10--> </InlineEquation>. Specifically, we derive new identities for the <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11957_2025_7227_Article_IEq5.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal{A}\)</EquationSource> <!--ContMath2460190Altwaijry-m11--> </InlineEquation>-numerical radius and provide further comparisons between the <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11957_2025_7227_Article_IEq5.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal{A}\)</EquationSource> <!--ContMath2460190Altwaijry-m12--> </InlineEquation>-numerical radius and the operator <InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11957_2025_7227_Article_IEq5.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal{A}\)</EquationSource> <!--ContMath2460190Altwaijry-m13--> </InlineEquation>-seminorm of weighted real and weighted imaginary parts. Additionally, we utilize Boas–Bellman type inequalities in the context of semi-Hilbert spaces to derive upper bounds for <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11957_2025_7227_Article_IEq8.gif" Format="GIF" Height="21" Rendition="HTML" Resolution="72" Type="Linedraw" Width="60" /> </InlineMediaObject> <EquationSource Format="TEX">\(\omega_{(\varepsilon,\mathcal{A})}\left(\cdot\right)\)</EquationSource> <!--ContMath2460190Altwaijry-m14--> </InlineEquation>. Several applications are also discussed.</p>

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(\({\varepsilon}\), \(\boldsymbol{\mathcal{A}}\))-Numerical Radius of Operators and Related Inequalities

  • N. Altwaijry,
  • S. S. Dragomir,
  • K. Feki,
  • H. Qiao

摘要

Abstract

The concept of the weighted \(\mathcal{A}\) -numerical radius was recently defined, where \(\mathcal{A}\) is assumed to be a positive operator. In this paper, we introduce another weighted \(\mathcal{A}\) -numerical radius, denoted by \(\omega_{(\varepsilon,\mathcal{A})}\left(\cdot\right)\) , for operators in semi-Hilbert spaces. We establish some basic properties and inequalities for \(\omega_{(\varepsilon,\mathcal{A})}\left(\cdot\right)\) , which generalize earlier results about \(\omega_{\mathcal{A}}(\cdot)\) . Specifically, we derive new identities for the \(\mathcal{A}\) -numerical radius and provide further comparisons between the \(\mathcal{A}\) -numerical radius and the operator \(\mathcal{A}\) -seminorm of weighted real and weighted imaginary parts. Additionally, we utilize Boas–Bellman type inequalities in the context of semi-Hilbert spaces to derive upper bounds for \(\omega_{(\varepsilon,\mathcal{A})}\left(\cdot\right)\) . Several applications are also discussed.