<p>We study the Cauchy problem for a mixed-sign quadratic Dirac equation on a noncompact <i>N</i>–star metric graph <i>G</i>, <Equation ID="Equ30"> <EquationSource Format="TEX">\( \textrm{i}\partial _t \psi = D\psi - \mathcal {N}(\psi ), \qquad \psi (0)=\psi _0, \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtext>i</mtext> <msub> <mi>∂</mi> <mi>t</mi> </msub> <mi>ψ</mi> <mo>=</mo> <mi>D</mi> <mi>ψ</mi> <mo>-</mo> <mi mathvariant="script">N</mi> <mrow> <mo stretchy="false">(</mo> <mi>ψ</mi> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> <mspace width="2em" /> <mi>ψ</mi> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <msub> <mi>ψ</mi> <mn>0</mn> </msub> <mo>,</mo> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\psi =(\psi _1,\psi _2)^{\mathsf T}:\mathbb {R}\times G\rightarrow \mathbb {C}^2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ψ</mi> <mo>=</mo> <msup> <mrow> <mo stretchy="false">(</mo> <msub> <mi>ψ</mi> <mn>1</mn> </msub> <mo>,</mo> <msub> <mi>ψ</mi> <mn>2</mn> </msub> <mo stretchy="false">)</mo> </mrow> <mi mathvariant="sans-serif">T</mi> </msup> <mo>:</mo> <mi mathvariant="double-struck">R</mi> <mo>×</mo> <mi>G</mi> <mo stretchy="false">→</mo> <msup> <mrow> <mi mathvariant="double-struck">C</mi> </mrow> <mn>2</mn> </msup> </mrow> </math></EquationSource> </InlineEquation> and <i>D</i> denotes the self-adjoint Dirac–Kirchhoff operator on <i>G</i>. The nonlinearity acts edgewise and is given by a bilinear interaction between the positive and negative spectral parts, <Equation ID="Equ31"> <EquationSource Format="TEX">\( \mathcal {N}(\psi )=\mathcal {B}\bigl (\Pi _+\psi ,\Pi _-\psi \bigr ), \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mi mathvariant="script">N</mi> <mrow> <mo stretchy="false">(</mo> <mi>ψ</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <mi mathvariant="script">B</mi> <mrow> <mo maxsize="1.2em" minsize="1.2em" stretchy="true">(</mo> </mrow> <msub> <mi mathvariant="normal">Π</mi> <mo>+</mo> </msub> <mi>ψ</mi> <mo>,</mo> <msub> <mi mathvariant="normal">Π</mi> <mo>-</mo> </msub> <mi>ψ</mi> <mrow> <mo maxsize="1.2em" minsize="1.2em" stretchy="true">)</mo> </mrow> <mo>,</mo> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\Pi _\pm \)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="normal">Π</mi> <mo>±</mo> </msub> </math></EquationSource> </InlineEquation> are the spectral projections of <i>D</i> and <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\mathcal {B}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">B</mi> </math></EquationSource> </InlineEquation> is a fixed bilinear map on <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\mathbb {C}^2\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">C</mi> </mrow> <mn>2</mn> </msup> </math></EquationSource> </InlineEquation> applied componentwise on each edge. This is a model quadratic interaction tailored to the mixed-sign Bourgain-space mechanism, rather than a general nonlinear Dirac equation on graphs. Using Bourgain-type spaces associated with the spectral resolution of <i>D</i> and a mixed-sign bilinear estimate on <i>N</i>–star graphs, we prove local well-posedness in the operator Sobolev space <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(H_D^s(G)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>H</mi> <mi>D</mi> <mi>s</mi> </msubsup> <mrow> <mo stretchy="false">(</mo> <mi>G</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> for <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(s&gt;-\frac{1}{8}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>s</mi> <mo>&gt;</mo> <mo>-</mo> <mfrac> <mn>1</mn> <mn>8</mn> </mfrac> </mrow> </math></EquationSource> </InlineEquation>. We also establish a blow-up alternative in <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(H_D^s(G)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>H</mi> <mi>D</mi> <mi>s</mi> </msubsup> <mrow> <mo stretchy="false">(</mo> <mi>G</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> for the maximal forward lifespan.</p>

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Low-regularity well-posedness for a mixed-sign quadratic Dirac equation on N-star metric graphs

  • Huichao Xing,
  • Zhipeng Yang

摘要

We study the Cauchy problem for a mixed-sign quadratic Dirac equation on a noncompact N–star metric graph G, \( \textrm{i}\partial _t \psi = D\psi - \mathcal {N}(\psi ), \qquad \psi (0)=\psi _0, \) i t ψ = D ψ - N ( ψ ) , ψ ( 0 ) = ψ 0 , where \(\psi =(\psi _1,\psi _2)^{\mathsf T}:\mathbb {R}\times G\rightarrow \mathbb {C}^2\) ψ = ( ψ 1 , ψ 2 ) T : R × G C 2 and D denotes the self-adjoint Dirac–Kirchhoff operator on G. The nonlinearity acts edgewise and is given by a bilinear interaction between the positive and negative spectral parts, \( \mathcal {N}(\psi )=\mathcal {B}\bigl (\Pi _+\psi ,\Pi _-\psi \bigr ), \) N ( ψ ) = B ( Π + ψ , Π - ψ ) , where \(\Pi _\pm \) Π ± are the spectral projections of D and \(\mathcal {B}\) B is a fixed bilinear map on \(\mathbb {C}^2\) C 2 applied componentwise on each edge. This is a model quadratic interaction tailored to the mixed-sign Bourgain-space mechanism, rather than a general nonlinear Dirac equation on graphs. Using Bourgain-type spaces associated with the spectral resolution of D and a mixed-sign bilinear estimate on N–star graphs, we prove local well-posedness in the operator Sobolev space \(H_D^s(G)\) H D s ( G ) for \(s>-\frac{1}{8}\) s > - 1 8 . We also establish a blow-up alternative in \(H_D^s(G)\) H D s ( G ) for the maximal forward lifespan.