<p>We introduce the <i>Cayley–Dickson Fourier transform (CDFT)</i>, a novel framework for harmonic analysis of functions valued in the non-associative Cayley–Dickson algebras <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\( \mathcal {C}_m \)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="script">C</mi> <mi>m</mi> </msub> </math></EquationSource> </InlineEquation>. The central challenge lies in the failure of associativity and alternativity for <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\( m \geqslant 4 \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>m</mi> <mo>⩾</mo> <mn>4</mn> </mrow> </math></EquationSource> </InlineEquation>, which obstructs classical Fourier analytic methods. To overcome this, we develop a two-stage approach: first, we construct the transform on real-valued Schwartz-type spaces, establishing continuity, inversion, and isometric properties; second, we extend the theory to fully <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\( \mathcal {C}_m \)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="script">C</mi> <mi>m</mi> </msub> </math></EquationSource> </InlineEquation>-valued functions by leveraging intrinsic algebraic structures, such as slice-wise multiplicativity and weak commutativity. Key innovations include a modified duality between differentiation and multiplication, governed by twisted sign involutions that precisely compensate for non-associative distortions, and a restricted convolution theorem for Gaussian-type functions that exploits the real scalar structure of their transforms. We prove that the CDFT admits an explicit inverse via symmetrization over coordinate reflections, acts isometrically on <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\( L^2(\mathbb {R}^m, \mathcal {C}_m) \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>L</mi> <mn>2</mn> </msup> <mrow> <mo stretchy="false">(</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>m</mi> </msup> <mo>,</mo> <msub> <mi mathvariant="script">C</mi> <mi>m</mi> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, and exhibits a period-four symmetry that generalizes classical Fourier periodicity. These results collectively establish the CDFT as a rigorous and structurally faithful extension of Fourier analysis to the full Cayley–Dickson hierarchy.</p>

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Fourier Transform on Cayley–Dickson Algebras

  • Shihao Fan,
  • Guangbin Ren

摘要

We introduce the Cayley–Dickson Fourier transform (CDFT), a novel framework for harmonic analysis of functions valued in the non-associative Cayley–Dickson algebras \( \mathcal {C}_m \) C m . The central challenge lies in the failure of associativity and alternativity for \( m \geqslant 4 \) m 4 , which obstructs classical Fourier analytic methods. To overcome this, we develop a two-stage approach: first, we construct the transform on real-valued Schwartz-type spaces, establishing continuity, inversion, and isometric properties; second, we extend the theory to fully \( \mathcal {C}_m \) C m -valued functions by leveraging intrinsic algebraic structures, such as slice-wise multiplicativity and weak commutativity. Key innovations include a modified duality between differentiation and multiplication, governed by twisted sign involutions that precisely compensate for non-associative distortions, and a restricted convolution theorem for Gaussian-type functions that exploits the real scalar structure of their transforms. We prove that the CDFT admits an explicit inverse via symmetrization over coordinate reflections, acts isometrically on \( L^2(\mathbb {R}^m, \mathcal {C}_m) \) L 2 ( R m , C m ) , and exhibits a period-four symmetry that generalizes classical Fourier periodicity. These results collectively establish the CDFT as a rigorous and structurally faithful extension of Fourier analysis to the full Cayley–Dickson hierarchy.