2018
DOI: 10.1016/j.optcom.2017.11.035
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Coded diffraction system in X-ray crystallography using a boolean phase coded aperture approximation

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Cited by 17 publications
(13 citation statements)
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“…This limits its use for large scale scenes because of the expensive computational memory requirements and the potential overfitting problems [64]. We propose to reduce the number of trainable parameters by adding spatial structure to each CA so that a kernel Q s of size ∆ n × ∆ m N × M is periodically repeated as follows Number of snapshots in (10) Trainable parameters in (14) manufacturing noise in (16) Conditionality in (13) Multishot correlation in (12) 4. Regularizer Fig.…”
Section: F Data Driven Conditionality Constraintmentioning
confidence: 99%
See 1 more Smart Citation
“…This limits its use for large scale scenes because of the expensive computational memory requirements and the potential overfitting problems [64]. We propose to reduce the number of trainable parameters by adding spatial structure to each CA so that a kernel Q s of size ∆ n × ∆ m N × M is periodically repeated as follows Number of snapshots in (10) Trainable parameters in (14) manufacturing noise in (16) Conditionality in (13) Multishot correlation in (12) 4. Regularizer Fig.…”
Section: F Data Driven Conditionality Constraintmentioning
confidence: 99%
“…Analytically, the CA is modeled as a tensor array where each spatial location has a particular response to the incoming wavefront. According to the nature of the entry values they can be found polarizer CA [4], complex-modulating CA [10], phase CA [13], intensity-modulating CA [14], among others. This work focuses on CAs modulating the intensity through (i) binary CA (BCA) [15], with opaque and translucent elements that completely block or let pass the wavefront, and (ii) realvalued CA [16] that attenuates the wavefront at different levels.…”
Section: Introductionmentioning
confidence: 99%
“…where ℓ kt = ϕµ(|a H kt z|) − q kt 2 . Note that setting µ = 0 in (8) leads to the non-smooth problem in (3). Note also that recent works such as [9,15] have addressed the non-smoothness of g(z) in (4) by introducing truncation parameters into the gradient step in order to eliminate the errors in the estimated descent direction.…”
Section: Stochastic Smoothing Phase Retrieval Algorithmmentioning
confidence: 99%
“…Phase retrieval is an inverse problem that consists of recovering a signal from the squared modulus of some linear transforms, which has proved efficient in in various applications such as, optics [1], astronomy [2] and X-ray crystallography [3,4,5,6]. Recent works [7,8,9] have been proposed to solve the phase retrieval problem by optimizing a non-convex and non-smooth objective function with a gradient descent algorithm based on the Wirtinger derivative with an appropriate initialization.…”
Section: Introductionmentioning
confidence: 99%
“…In many applications of science and engineering, it is required to recover a signal from the squared modulus of any linear transform, which is known as phase retrieval (PR). Such a task is present in optics [1], astronomical imaging [2], microscopy [3] and x-ray crystallography [4,5,6], where the optical sensors measure the intensities of the reflection, but they are not able to measure the phase of the signal. For example, in x-ray crystallography [4], PR is used to determine the atomic position of a crystal in a three-dimensional (3D) space [7].…”
Section: Introductionmentioning
confidence: 99%