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Ball Stabilization in Inverse Problems

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Inverse Methods in Action

Part of the book series: Inverse Problems and Theoretical Imaging ((IPTI))

Abstract

We take as starting point a continuous, bijective map M from a Banach space C to a Banach space S 1) The inverse problem starts from an initial data function DD(s), which is a point in S, and seeks, by using a properly defined generalized inverse map M Q −1 to obtain as solution a well-defined function ϕ 22 ≡(t) belonging to C. Continuity of M does not ensure that the inverse map M −1 will be continuous (see Fig. I below); more generally the stabilization of the generalized (quasisolution) inverse map M Q −1 is a central element in solving the inverse problem. The need to introduce quasisolutions arises because D, although it belongs to S, may not be in M(C).

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References

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© 1990 Springer-Verlag Berlin Heidelberg

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Ciulli, M., Ciulli, S., Spearman, T.D. (1990). Ball Stabilization in Inverse Problems. In: Sabatier, P.C. (eds) Inverse Methods in Action. Inverse Problems and Theoretical Imaging. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-75298-8_17

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  • DOI: https://doi.org/10.1007/978-3-642-75298-8_17

  • Publisher Name: Springer, Berlin, Heidelberg

  • Print ISBN: 978-3-642-75300-8

  • Online ISBN: 978-3-642-75298-8

  • eBook Packages: Springer Book Archive

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