<p>The <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>α</mi> </math></EquationSource> </InlineEquation>-energy of a graph <i>G</i> with <i>n</i> vertices and <i>m</i> edges is defined by <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(E^{A_\alpha }(G)=\sum _{i=1}^n\left| \lambda _i^\alpha -\frac{2 \alpha m}{n}\right| \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>E</mi> <msub> <mi>A</mi> <mi>α</mi> </msub> </msup> <mrow> <mo stretchy="false">(</mo> <mi>G</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <msubsup> <mo>∑</mo> <mrow> <mi>i</mi> <mo>=</mo> <mn>1</mn> </mrow> <mi>n</mi> </msubsup> <mfenced close="|" open="|"> <msubsup> <mi>λ</mi> <mi>i</mi> <mi>α</mi> </msubsup> <mo>-</mo> <mfrac> <mrow> <mn>2</mn> <mi>α</mi> <mi>m</mi> </mrow> <mi>n</mi> </mfrac> </mfenced> </mrow> </math></EquationSource> </InlineEquation>, where <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\lambda _i^\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi>λ</mi> <mi>i</mi> <mi>α</mi> </msubsup> </math></EquationSource> </InlineEquation> denotes the <i>i</i>-th largest eigenvalue of the <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(A_\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>A</mi> <mi>α</mi> </msub> </math></EquationSource> </InlineEquation>-matrix of <i>G</i>. In this paper, we first establish a sharp lower bound for the <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(A_\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>A</mi> <mi>α</mi> </msub> </math></EquationSource> </InlineEquation>-spectral radius of a graph in terms of its degree and average 2-degree, thereby refining and extending the classical bound <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(\lambda _1^\alpha (G)\ge \tfrac{1}{2}\Big (\alpha (\Delta +1)+\sqrt{\alpha ^2(\Delta +1)^2+4\Delta (1-2\alpha )}\Big )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>λ</mi> <mn>1</mn> <mi>α</mi> </msubsup> <mrow> <mo stretchy="false">(</mo> <mi>G</mi> <mo stretchy="false">)</mo> </mrow> <mo>≥</mo> <mstyle displaystyle="false" scriptlevel="0"> <mfrac> <mn>1</mn> <mn>2</mn> </mfrac> </mstyle> <mrow> <mo maxsize="1.623em" minsize="1.623em" stretchy="true">(</mo> </mrow> <mi>α</mi> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">Δ</mi> <mo>+</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> <mo>+</mo> <msqrt> <mrow> <msup> <mi>α</mi> <mn>2</mn> </msup> <msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="normal">Δ</mi> <mo>+</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> <mn>2</mn> </msup> <mo>+</mo> <mn>4</mn> <mi mathvariant="normal">Δ</mi> <mrow> <mo stretchy="false">(</mo> <mn>1</mn> <mo>-</mo> <mn>2</mn> <mi>α</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </msqrt> <mrow> <mo maxsize="1.623em" minsize="1.623em" stretchy="true">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. As applications, we derive tight lower and upper bounds on the <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>α</mi> </math></EquationSource> </InlineEquation>-energy of connected graphs and provide a complete characterization of all extremal graphs attaining these bounds. Our results unify and generalize several existing conclusions, including the signless Laplacian energy bounds of Chen et al.&#xa0;(2026) and the <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>α</mi> </math></EquationSource> </InlineEquation>-energy bounds of Pirzada et al.&#xa0;(2021).</p>

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The \(\alpha \)-energy and \(A_\alpha \)-spectral radius of a graph

  • Long Jin

摘要

The \(\alpha \) α -energy of a graph G with n vertices and m edges is defined by \(E^{A_\alpha }(G)=\sum _{i=1}^n\left| \lambda _i^\alpha -\frac{2 \alpha m}{n}\right| \) E A α ( G ) = i = 1 n λ i α - 2 α m n , where \(\lambda _i^\alpha \) λ i α denotes the i-th largest eigenvalue of the \(A_\alpha \) A α -matrix of G. In this paper, we first establish a sharp lower bound for the \(A_\alpha \) A α -spectral radius of a graph in terms of its degree and average 2-degree, thereby refining and extending the classical bound \(\lambda _1^\alpha (G)\ge \tfrac{1}{2}\Big (\alpha (\Delta +1)+\sqrt{\alpha ^2(\Delta +1)^2+4\Delta (1-2\alpha )}\Big )\) λ 1 α ( G ) 1 2 ( α ( Δ + 1 ) + α 2 ( Δ + 1 ) 2 + 4 Δ ( 1 - 2 α ) ) . As applications, we derive tight lower and upper bounds on the \(\alpha \) α -energy of connected graphs and provide a complete characterization of all extremal graphs attaining these bounds. Our results unify and generalize several existing conclusions, including the signless Laplacian energy bounds of Chen et al. (2026) and the \(\alpha \) α -energy bounds of Pirzada et al. (2021).