<p>Let <i>K</i> and <i>L</i> be two convex bodies in <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2000_Article_IEq4.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathbb {R}}^4\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>4</mn> </msup> </math></EquationSource> </InlineEquation>, such that their orthogonal projections onto every 3-dimensional subspace are rotations of each other or reflections with respect to a 2-dimensional plane in the subspace. Assume also that the complex lines (we identify <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2000_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <EquationSource Format="TEX">\({\mathbb {R}^4}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>4</mn> </msup> </math></EquationSource> </InlineEquation> with <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2000_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="18" /> </InlineMediaObject> <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>) are the invariant subspaces of the corresponding rotations or reflections. Then <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="12220_2025_2000_Article_IEq7.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="54" /> </InlineMediaObject> <EquationSource Format="TEX">\(K=L\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>K</mi> <mo>=</mo> <mi>L</mi> </mrow> </math></EquationSource> </InlineEquation>. A similar statement is proved for sections of <i>K</i> and <i>L</i>.</p>

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On Pairs of Bodies in \({\mathbb {R}^4}\) with Congruent Sections or Projections

  • Reema A. Sbeih

摘要

Let K and L be two convex bodies in \({\mathbb {R}}^4\) R 4 , such that their orthogonal projections onto every 3-dimensional subspace are rotations of each other or reflections with respect to a 2-dimensional plane in the subspace. Assume also that the complex lines (we identify \({\mathbb {R}^4}\) R 4 with \({\mathbb {C}^2}\) C 2 ) are the invariant subspaces of the corresponding rotations or reflections. Then \(K=L\) K = L . A similar statement is proved for sections of K and L.