<p>For a genuinely nonlinear <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(2\times 2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>2</mn> <mo>×</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation> hyperbolic system of conservation laws, assuming that the initial data have a small <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\textbf{L}^\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi mathvariant="bold">L</mi> <mi>∞</mi> </msup> </math></EquationSource> </InlineEquation> norm but a possibly unbounded total variation, the existence of global solutions was proven in a classical paper by Glimm and Lax (1970). In general, the total variation of these solutions decays like <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(t^{-1}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>t</mi> <mrow> <mo>-</mo> <mn>1</mn> </mrow> </msup> </math></EquationSource> </InlineEquation>. Motivated by the theory of fractional domains for linear analytic semigroups, we consider here solutions with a faster decay rate: <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\hbox {Tot.Var.}\bigl \{u(t,\cdot )\bigr \}\le C t^{\alpha -1}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mtext>Tot.Var.</mtext> <mrow> <mo maxsize="1.2em" minsize="1.2em" stretchy="true">{</mo> </mrow> <mi>u</mi> <mrow> <mo stretchy="false">(</mo> <mi>t</mi> <mo>,</mo> <mo>·</mo> <mo stretchy="false">)</mo> </mrow> <mrow> <mo maxsize="1.2em" minsize="1.2em" stretchy="true">}</mo> </mrow> <mo>≤</mo> <mi>C</mi> <msup> <mi>t</mi> <mrow> <mi>α</mi> <mo>-</mo> <mn>1</mn> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation>. For these solutions, a uniqueness theorem is proven. Indeed, as the initial data range over a domain of functions with <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\Vert {\bar{u}}\Vert _{\textbf{L}^\infty } \le \varepsilon _1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mrow> <mo stretchy="false">‖</mo> <mover accent="true"> <mrow> <mi>u</mi> </mrow> <mrow> <mo stretchy="false">¯</mo> </mrow> </mover> <mo stretchy="false">‖</mo> </mrow> <msup> <mi mathvariant="bold">L</mi> <mi>∞</mi> </msup> </msub> <mo>≤</mo> <msub> <mi>ε</mi> <mn>1</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> small enough, solutions with a fast decay yield a Hölder continuous semigroup. The Hölder exponent can be taken arbitrarily close to 1 by further shrinking the value of <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(\varepsilon _1&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>ε</mi> <mn>1</mn> </msub> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>. An auxiliary result identifies a class of initial data whose solutions have rapidly decaying total variation.</p>

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Uniqueness Domains for \(\textbf{L}^\infty \) Solutions of \(2\times 2\) Hyperbolic Conservation Laws

  • Alberto Bressan,
  • Elio Marconi,
  • Ganesh Vaidya

摘要

For a genuinely nonlinear \(2\times 2\) 2 × 2 hyperbolic system of conservation laws, assuming that the initial data have a small \(\textbf{L}^\infty \) L norm but a possibly unbounded total variation, the existence of global solutions was proven in a classical paper by Glimm and Lax (1970). In general, the total variation of these solutions decays like \(t^{-1}\) t - 1 . Motivated by the theory of fractional domains for linear analytic semigroups, we consider here solutions with a faster decay rate: \(\hbox {Tot.Var.}\bigl \{u(t,\cdot )\bigr \}\le C t^{\alpha -1}\) Tot.Var. { u ( t , · ) } C t α - 1 . For these solutions, a uniqueness theorem is proven. Indeed, as the initial data range over a domain of functions with \(\Vert {\bar{u}}\Vert _{\textbf{L}^\infty } \le \varepsilon _1\) u ¯ L ε 1 small enough, solutions with a fast decay yield a Hölder continuous semigroup. The Hölder exponent can be taken arbitrarily close to 1 by further shrinking the value of \(\varepsilon _1>0\) ε 1 > 0 . An auxiliary result identifies a class of initial data whose solutions have rapidly decaying total variation.