2020
DOI: 10.3390/s20113147
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Speckle-Correlation Scattering Matrix Approaches for Imaging and Sensing through Turbidity

Abstract: The development of optical and computational techniques has enabled imaging without the need for traditional optical imaging systems. Modern lensless imaging techniques overcome several restrictions imposed by lenses, while preserving or even surpassing the capability of lens-based imaging. However, existing lensless methods often rely on a priori information about objects or imaging conditions. Thus, they are not ideal for general imaging purposes. The recent development of the speckle-correlation scattering … Show more

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Cited by 12 publications
(7 citation statements)
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References 102 publications
(143 reference statements)
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“…From the measured speckle pattern, the SSM method is applied using the designed TM. [ 9,10 ] To describe the reconstruction sequence, let us consider the orthonormal basis of the input field, U=false{e1,e2,,eNfalse}$U = \{{\bf{e}}_1,{\bf{e}}_2,\ldots,{\bf{e}}_N\}$. The basis can freely be defined such that it satisfies boldx=i=1Nxiboldei${\bf{x}} = \sum\nolimits_{i = 1}^N {{x_i}{{\bf{e}}_i}}$, where boldxCN${\bf x}\in {\mathbb C}^{N}$ is an unknown input field.…”
Section: Resultsmentioning
confidence: 99%
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“…From the measured speckle pattern, the SSM method is applied using the designed TM. [ 9,10 ] To describe the reconstruction sequence, let us consider the orthonormal basis of the input field, U=false{e1,e2,,eNfalse}$U = \{{\bf{e}}_1,{\bf{e}}_2,\ldots,{\bf{e}}_N\}$. The basis can freely be defined such that it satisfies boldx=i=1Nxiboldei${\bf{x}} = \sum\nolimits_{i = 1}^N {{x_i}{{\bf{e}}_i}}$, where boldxCN${\bf x}\in {\mathbb C}^{N}$ is an unknown input field.…”
Section: Resultsmentioning
confidence: 99%
“…[ 3 ] To address this, various reference‐free holographic imaging techniques have been developed. [ 4–9 ] Because phase is not a directly measurable quantity, most reference‐free phase imaging methods must either make a priori constraints on an input field or conduct multiple measurements. For example, coherent diffractive imaging utilizes sample support, [ 4 ] integration methods assume a well‐defined phase (no dark points) over the entire field of view, [ 5 ] and the transport of intensity equation methods [ 6 ] and ptychography exploit axial and lateral sample scanning to increase the number of sampling points.…”
Section: Introductionmentioning
confidence: 99%
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“…In CSI, we transform the sample field into a random speckle before the measurement using an X-ray diffuser 36 . Although the phase of the speckle is immeasurable either, the complex-valued sample field can be uniquely reconstructed from the magnitude image through the pseudorandomness of speckle [37][38][39][40] . Our CSI exploits a designed X-ray diffuser after the sample instead of a zone plate (Fig.…”
Section: Introductionmentioning
confidence: 99%
“…This method requires auxiliary equipment in most cases, which limits its application in practice. Speckle correlation imaging [10][11][12] based on the "memory effect" [13] of the scattering medium has also attracted research interest. The experimental requirements of speckle-related methods are relatively simple, but the imaging field of view is limited by the memory effect range, which is inversely proportional to the medium thickness.…”
Section: Introductionmentioning
confidence: 99%