<p>We study the ray transform <i>L</i> over null (light) rays in the pseudo-Euclidean space with signature <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2086_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="52" /> </InlineMediaObject> <EquationSource Format="TEX">\((n',n'')\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <msup> <mi>n</mi> <mo>′</mo> </msup> <mo>,</mo> <msup> <mi>n</mi> <mrow> <mo>′</mo> <mo>′</mo> </mrow> </msup> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2086_Article_IEq2.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="46" /> </InlineMediaObject> <EquationSource Format="TEX">\(n'\ge 2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>n</mi> <mo>′</mo> </msup> <mo>≥</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2086_Article_IEq3.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="50" /> </InlineMediaObject> <EquationSource Format="TEX">\(n''\ge 2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>n</mi> <mrow> <mo>′</mo> <mo>′</mo> </mrow> </msup> <mo>≥</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>. We analyze the normal operator <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2086_Article_IEq4.gif" Format="GIF" Height="15" Rendition="HTML" Resolution="72" Type="Linedraw" Width="31" /> </InlineMediaObject> <EquationSource Format="TEX">\(L'L\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mo>′</mo> </msup> <mi>L</mi> </mrow> </math></EquationSource> </InlineEquation>, derive an inversion formula, and prove stability estimates. We show that the symbol <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2086_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="32" /> </InlineMediaObject> <EquationSource Format="TEX">\(p(\xi )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo stretchy="false">(</mo> <mi>ξ</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> is elliptic but singular at the light cone <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2086_Article_IEq6.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathcal {L}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">L</mi> </math></EquationSource> </InlineEquation> with conormal singularities there. We analyze <i>L</i> as a Fourier Integral Operator as well. Finally, we compare this to the Minkowski case.</p>

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The Light Ray Transform for Pseudo-Euclidean Metrics

  • Divyansh Agrawal,
  • Plamen Stefanov

摘要

We study the ray transform L over null (light) rays in the pseudo-Euclidean space with signature \((n',n'')\) ( n , n ) , \(n'\ge 2\) n 2 , \(n''\ge 2\) n 2 . We analyze the normal operator \(L'L\) L L , derive an inversion formula, and prove stability estimates. We show that the symbol \(p(\xi )\) p ( ξ ) is elliptic but singular at the light cone \(\mathcal {L}\) L with conormal singularities there. We analyze L as a Fourier Integral Operator as well. Finally, we compare this to the Minkowski case.