Abstract
One well-known integral condition for a function to be holomorphic is the following classical Morera theorem: if a function \(f:\mathcal{O} \to \mathbb{C}\) is continuous in a domain \(\mathcal{O} \subset \mathbb{C}\) and has zero integrals over all rectifiable contours in \(\mathcal{O}\), then \(f\) is holomorphic in \(\mathcal{O}\). This fact allows for far-reaching generalizations in various directions. In particular, if a continuous function \(f:\mathbb{C} \to \mathbb{C}\) has zero integrals over all circles of fixed radii \({{r}_{1}}\) and \({{r}_{2}}\) in \(\mathbb{C}\) and \({{r}_{1}}{\text{/}}{{r}_{2}}\) is not the ratio of two zeros of the Bessel function \({{J}_{1}}\), then \(f\) is holomorphic on the whole complex plane (entire). One example of the function \(\frac{\partial }{{\partial z}}\left( {{{J}_{0}}\left( {\lambda \left| z \right|} \right)} \right)\) with a suitable parameter \(\lambda \) shows that this condition on \({{r}_{1}}{\text{/}}{{r}_{2}}\) cannot be omitted. In this article, we study the problem of recovering the derivative \(\frac{{\partial f}}{{\partial \bar {z}}}\) from given contour integrals of \(f\). Our main result is Theorem 4, which gives a new formula for finding \(\frac{{\partial f}}{{\partial \bar {z}}}\) in terms of integrals of \(f\) over circles with the above condition. The key step in the proof of Theorem 4 is the expansion of the Dirac delta function in terms of a system of radial distributions supported in \({{\bar {B}}_{r}}\) biorthogonal to some system of spherical functions. A similar approach can be used to invert a number of convolution operators with radial distributions in \(\mathcal{E}{\kern 1pt} '{\kern 1pt} ({{\mathbb{C}}^{n}})\).
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Translated by E. Seifina
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Volchkova, N.P., Volchkov, V.V. Reconstruction of the Cauchy–Riemann Operator by Complex Integration Operators along Circles. Russ Math. 67, 16–28 (2023). https://doi.org/10.3103/S1066369X23050109
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DOI: https://doi.org/10.3103/S1066369X23050109