Linnik point spread functions, time-reversed logarithmic diffusion equations, and blind deconvolution of electron microscope imagery
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| Format: | Preprint |
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2025
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| author | Carasso, Alfred S. Vladar, Andras E. |
| author_facet | Carasso, Alfred S. Vladar, Andras E. |
| contents | A non iterative direct blind deconvolution procedure, previously used successfully to sharpen Hubble Space Telescope imagery, is now found useful in sharpening nanoscale scanning electron microscope (SEM) and helium ion microscope (HIM) images. The method is restricted to images $g(x,y)$, whose Fourier transforms $\hat{g}(ξ,η)$ are such that $log~|\hat{g}(ξ,0)|$ is globally monotone decreasing and convex. The method is not applicable to defocus blurs. A point spread function in the form of a Linnik probability density function is postulated, with parameters obtained by least squares fitting the Fourier transform of the preconditioned microscopy image. Deconvolution is implemented in slow motion by marching backward in time, in Fourier space, from $t = 1$ to $t = 0$, in an associated logarithmic diffusion equation. Best results are usually found in a partial deconvolution at time $\bar{t}$, with $0 < \bar{t} < 1$, rather than in total deconvolution at $t=0$. The method requires familarity with microscopy images, as well as interactive search for optimal parameters. |
| format | Preprint |
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arxiv_https___arxiv_org_abs_2502_19420 |
| institution | arXiv |
| publishDate | 2025 |
| record_format | arxiv |
| spellingShingle | Linnik point spread functions, time-reversed logarithmic diffusion equations, and blind deconvolution of electron microscope imagery Carasso, Alfred S. Vladar, Andras E. Instrumentation and Detectors Instrumentation and Methods for Astrophysics Numerical Analysis Optics A non iterative direct blind deconvolution procedure, previously used successfully to sharpen Hubble Space Telescope imagery, is now found useful in sharpening nanoscale scanning electron microscope (SEM) and helium ion microscope (HIM) images. The method is restricted to images $g(x,y)$, whose Fourier transforms $\hat{g}(ξ,η)$ are such that $log~|\hat{g}(ξ,0)|$ is globally monotone decreasing and convex. The method is not applicable to defocus blurs. A point spread function in the form of a Linnik probability density function is postulated, with parameters obtained by least squares fitting the Fourier transform of the preconditioned microscopy image. Deconvolution is implemented in slow motion by marching backward in time, in Fourier space, from $t = 1$ to $t = 0$, in an associated logarithmic diffusion equation. Best results are usually found in a partial deconvolution at time $\bar{t}$, with $0 < \bar{t} < 1$, rather than in total deconvolution at $t=0$. The method requires familarity with microscopy images, as well as interactive search for optimal parameters. |
| title | Linnik point spread functions, time-reversed logarithmic diffusion equations, and blind deconvolution of electron microscope imagery |
| topic | Instrumentation and Detectors Instrumentation and Methods for Astrophysics Numerical Analysis Optics |
| url | https://arxiv.org/abs/2502.19420 |