DOCSLIB.ORG

The Geometry of the Phase Retrieval Problem Charles L

Total Page：16

File Type：pdf, Size：1020Kb

Download full-text PDF Read full-text
The Geometry of the Phase Retrieval Problem Charles L The Geometry of the Phase Retrieval Problem Charles L. Epstein The Geometry of the Phase Retrieval Problem Introduction Operator Splitting Methods in Data Analysis Workshop Discrete Problem Torus Geometry Reconstruction Charles L. Epstein Algorithms Numerical Examples CCM at the Flatiron Institute University of Pennsylvania Other Conditions History of CDI March 20, 2019 Bibliography Acknowledgment The Geometry of the Phase Retrieval Problem Charles L. Epstein I want to thank Christian and Patrick for inviting me to speak. Introduction What I will discuss today is somewhat unconventional, ongoing Discrete Problem work, at the intersection of pure mathematics, numerical analysis Torus Geometry and mathematical physics. Reconstruction Algorithms This work was done jointly with Alex Barnett, Leslie Greengard, Numerical and Jeremy Magland and supported by the Centers for Examples Computational Biology and Mathematics at the Flatiron Institute Other Conditions of the Simons Foundation, New York, NY. History of CDI Bibliography Outline The Geometry of the Phase Retrieval Problem 1 Introduction Charles L. Epstein 2 The Discrete Phase Retrieval Problem Introduction 3 Geometry of the Torus Discrete Problem Torus Geometry 4 Reconstruction Algorithms Reconstruction Algorithms 5 Numerical Examples in Phase Retrieval Numerical Examples 6 Other Auxiliary Conditions Other Conditions History of CDI 7 Short History of CDI Bibliography 8 Bibliography High Resolution Imaging The Geometry of the Phase Retrieval Problem Charles L. Epstein Introduction Today I will speak about inverse problems that arise in Coherent Discrete Problem Diffraction Imaging. This is a technique that uses very high Torus Geometry energy, monochromatic light, either electrons or x-rays, to form Reconstruction high resolution images of animate and inanimate materials. The Algorithms goal is to achieve resolutions in the 1–10nm range. Numerical Examples Other Conditions History of CDI Bibliography What is Measured? The Geometry of the Phase Retrieval Problem Charles L. The photons used to illuminate the samples are in the 0.1-10KeV Epstein range; the light is typically assumed to be monochromatic, Introduction produced either by a laser or as synchrotron radiation. The object Discrete being imaged is typically many wavelengths across and the Problem measurement is made very far from the object and light source, Torus Geometry Reconstruction hence in the far field (the Fraunhofer regime). As is well known, Algorithms if .x/ describes the density of the object, then the leading order Numerical Examples term in the far field expansion of the scattered radiation is .k/; : Other proportional to the square of the Fourier transform, b of At Conditions such small wavelengths, one can only measure the intensity of the History of CDI 2 scattered field, b.k/ ; and not its phase. Bibliography j j Examples, I The Geometry of the Phase Retrieval Here are computed far field diffraction patterns produced by (a) a Problem semi-circle, (b) an equilateral triangle. Charles L. Epstein Introduction Discrete Problem Torus Geometry Reconstruction Algorithms Numerical Examples Other Conditions History of CDI Bibliography Examples, II FROZEN-HYDRATED YEAST SPORES RECONSTRUCTION The Geometry of the Phase Here is an actual diffraction• E. Lima, patternPhD Thesis, produced Stony Brook by frozen-hydrated University Retrieval Problem yeast spore at 520• eV.Unstained Courtesy frozen-hydrated E. Lima PhD yeast thesis, spore, Stony at 520 Brook eV Charles L. U, from [8]. Epstein • First CDI reconstruction of a frozen hydrated biological object Introduction Discrete Problem Torus Geometry Reconstruction Algorithms Numerical Examples Other Conditions History of CDI Bibliography Signal extends to 25 nm Brightness - amplitude half-period Hue - phase ESRF Lecture Series on Coherent X-rays and their Applications, Lecture 7, Malcolm Howells What is Needed? The Geometry .x/ of the Phase Of course we would like to reconstruct from this Retrieval Problem measurement, but we need to, at least, estimate the unmeasured Charles L. phase of b.k/: This is called the phase retrieval problem. Epstein It also arises in x-ray crystallography, but is really quite a different Introduction problem for a periodic structure. In the context of a compact Discrete object, the possibility of solving this problem was first suggested Problem Torus Geometry by D. Sayre in 1952. He saw it as a consequence of Nyquist’s Reconstruction sampling theorem! See [1]. Algorithms For this problem to be solvable, even in principle, some auxiliary Numerical Examples information is required, such as an estimate for the support of the Other object, or knowledge that the function .x/ is non-negative and an Conditions estimate on the support of its autocorrelation function. History of CDI Bibliography Many attempts have been made to solve this problem, but with rather limited success. Today we’ll discuss the underlying reasons for the difficulty of this problem...which may suggest better approaches. Outline of this Lecture The Geometry of the Phase Retrieval Problem Charles L. Epstein Introduction We will try to cover to following material: Discrete Problem The Discrete Phase Retrieval Problem (a simpler model) Torus Geometry Geometry of the Amplitude Torus Reconstruction Algorithms Reconstruction Algorithms Numerical What We Learn from Numerical Examples Examples Other Conditions History of CDI Bibliography Outline The Geometry of the Phase Retrieval Problem 1 Introduction Charles L. Epstein 2 The Discrete Phase Retrieval Problem Introduction 3 Geometry of the Torus Discrete Problem Torus Geometry 4 Reconstruction Algorithms Reconstruction Algorithms 5 Numerical Examples in Phase Retrieval Numerical Examples 6 Other Auxiliary Conditions Other Conditions History of CDI 7 Short History of CDI Bibliography 8 Bibliography A Simpler Model Problem The Geometry of the Phase Retrieval Problem Charles L. The phase retrieval problem encountered in coherent diffraction Epstein imaging is fraught with many practical difficulties. For the Introduction remainder of the talk we focus on a simpler model problem, which Discrete Problem already proves very difficult to solve. We call this the discrete, Torus Geometry classical phase retrieval problem. We imagine that the unknowns Reconstruction are samples of an object on a finite uniform grid: Algorithms Numerical xj .j1x; j2x/; where j J: (1) Examples D 2 Other Conditions Here J Œn1 N1 Œn2 N2; is a rectangular grid. We call D W W History of CDI such collections of data indexed by J images. Bibliography The Measurements The Geometry of the Phase In our model problem, the measured data are the magnitudes of Retrieval Problem the DFT of these samples: Charles L. Epstein aj xj j bJ ; (2) f D j O j W 2 g Introduction where bJ is a set of sample frequencies, with J bJ : If Discrete d j j D j j Problem J Œ0 N 1 ; then D W Torus Geometry X 2ij k N Reconstruction xj xke : (3) Algorithms O D k J Numerical 2 Examples We let RJ RJ denote the measurement map: Other M W ! Conditions C History of CDI .x/ . xj /j J : (4) M D j O j 2 Bibliography There are important differences between these model measurements and the samples of a continuum Fourier transform that would actually be collected. The Support Condition, I The Geometry of the Phase As noted above we need to have auxiliary information to be able Retrieval Problem to solve the phase retrieval problem. We imagine that the support Charles L. x;S ; Epstein of the unknown image x is contained in a rectangular subset R J with the side lengths of R at most half those of J: In the Introduction literature it is often said that we “oversample,” but really we just Discrete Problem need to sample in k-space on a fine enough grid for the data set to Torus Geometry contain information about the support of x: Reconstruction Algorithms Our auxiliary information will be an estimate for Sx: This is a Numerical subset S with Sx S R J: We are therefore looking for an Examples image x so that xj 0 for j S; and Other D … Conditions History of CDI xj aj for all j bJ: (5) j O j D 2 Bibliography This problem usually does not have a unique solution, but generically, the non-uniqueness is of a simple sort. Trivial Associates The Geometry of the Phase Retrieval Problem x J; Charles L. If is an image indexed by then we think of it as being Epstein periodic in Z2; with j J representing a single period cell. We f 2 g can then translate an image by any lattice vector k Z2; defining Introduction 2 Discrete Problem .k/ d xj xj k: (6) Torus Geometry D Reconstruction Algorithms We can also define the inverted image by setting Numerical Examples xj x j : (7) Other L D Conditions History of CDI Translation and inversion lead to images with the same magnitude Bibliography Fourier data; these are called the trivial associates of x: Uniqueness The Geometry of the Phase Retrieval Hence there are always many images with the same magnitude Problem R; Charles L. Fourier data, and support in a translate of but there is a Epstein theorem, due to Monson Hayes (see [5]) which states that Introduction generically this is the only form of non-uniqueness one Discrete encounters: with sufficiently fine sampling in the Fourier domain, Problem the only images with the given magnitude Fourier data are the Torus Geometry trivial associates of a given image with this data. Reconstruction Algorithms Let Sx S R; as above; the support condition S defines a Numerical J Examples linear subspace of R ; Other Conditions J BS x R xj 0 if j S : (8) History of CDI D f 2 W D … g Bibliography 1 In all cases . .x// BS is a finite set, and generically it M M \ consists of trivial associates of x: The Support Condition, II The Geometry of the Phase Retrieval Problem The better our estimate, S; for the support is, the fewer trivial Charles L.
Load more

Recommended publications
  • Aspects of Phase Retrieval in X-Ray Crystallography
    Aspects of Phase Retrieval in X-ray Crystallography Romain Arnal A thesis presented for the degree of Doctor of Philosophy in Electrical and Computer Engineering at the University of Canterbury, Christchurch, New Zealand. June 2019 Deputy Vice-Chancellor’s Office Postgraduate Office Co-Authorship Form This form is to accompany the submission of any thesis that contains research reported in co- authored work that has been published, accepted for publication, or submitted for publication. A copy of this form should be included for each co-authored work that is included in the thesis. Completed forms should be included at the front (after the thesis abstract) of each copy of the thesis submitted for examination and library deposit. Please indicate the chapter/section/pages of this thesis that are extracted from co-authored work and provide details of the publication or submission from the extract comes: Chapter 2 describes work by the candidate that is reported in “Millane and Arnal, Uniqueness of the macromolecular crystallographic phase problem, Acta Cryst., A71, 592-598, 2015.” Please detail the nature and extent (%) of contribution by the candidate: This publication describes joint work by the candidate and Millane. The theory was derived jointly by the candidate and Millane. The simulations, the required software development, and presentation of the results were conducted by the candidate. Writing was a joint effort. Certification by Co-authors: If there is more than one co-author then a single co-author can sign on behalf of all The
    [Show full text]
  • Iterative Phase Retrieval in Coherent Diffractive Imaging: Practical Issues
    Iterative phase retrieval in coherent diffractive imaging: practical issues Tatiana Latychevskaia, [email protected] ABSTRACT In this work, issues in phase retrieval in the coherent diffractive imaging (CDI) technique, from discussion on parameters for setting up a CDI experiment to evaluation of the goodness of the final reconstruction, are discussed. The distribution of objects under study by CDI often cannot be cross- validated by another imaging technique. It is therefore important to make sure that the developed CDI procedure delivers an artifact-free object reconstruction. Critical issues that can lead to artifacts are presented and recipes on how to avoid them are provided. Contents Iterative phase retrieval in coherent diffractive imaging: practical issues ............................................. 1 1. Introduction ......................................................................................................................................... 3 2. Basics of CDI experiment ..................................................................................................................... 3 2.1. Diffraction pattern formation ...................................................................................................... 3 2.2 Oversampling ................................................................................................................................. 6 2.3 Iterative phase-retrieval algorithms .............................................................................................. 7 2.3.1
    [Show full text]
  • Low-Rank Fourier Ptychography
    LOW RANK FOURIER PTYCHOGRAPHY Zhengyu Chen, Gauri Jagatap, Seyedehsara Nayer, Chinmay Hegde, Namrata Vaswani Iowa State University ABSTRACT reconstruction problem is nascent, and several important questions remain unanswered. Rigorous guarantees of correctness of the meth- In this paper, we introduce a principled algorithmic approach for ods proposed in [8, 10] are not yet available. More worrisome is the Fourier ptychographic imaging of dynamic, time-varying targets. To issue of sample complexity of image reconstruction, since a basic the best of our knowledge, this setting has not been explicitly ad- requirement in all existing methods is that the number of measure- dressed in the ptychography literature. We argue that such a setting ments must exceed the resolution of the image. However, this re- is very natural, and that our methods provide an important first step quirement can be particularly challenging when imaging a dynamic towards helping reduce the sample complexity (and hence acquisi- scene involving a moving target; for a video sequence with q images tion time) of imaging dynamic scenes to managaeble levels. With each with resolution n, without using any structural prior assump- significantly reduced acquisition times per image, it is conceivable tions, the number of observations must be at least Ω(nq), which can that dynamic ptychographic imaging of fast changing scenes indeeed quickly become prohibitive. becomes practical in the near future. Index Terms— Phase retrieval, ptychography, low rank 1.2. Our Contributions 1. INTRODUCTION In this paper, we introduce a principled algorithmic approach for Fourier ptychographic imaging of dynamic, time-varying targets. To 1.1. Motivation the best of our knowledge, this setting has not been explicitly ad- dressed in the ptychography literature.
    [Show full text]
  • The Numerics of Phase Retrieval
    THE NUMERICS OF PHASE RETRIEVAL ALBERT FANNJIANG AND THOMAS STROHMER Abstract. Phase retrieval, i.e., the problem of recovering a function from the squared magnitude of its Fourier transform, arises in many applications such as X-ray crystallog- raphy, diffraction imaging, optics, quantum mechanics, and astronomy. This problem has confounded engineers, physicists, and mathematicians for many decades. Recently, phase re- trieval has seen a resurgence in research activity, ignited by new imaging modalities and novel mathematical concepts. As our scientific experiments produce larger and larger datasets and we aim for faster and faster throughput, it becomes increasingly important to study the involved numerical algorithms in a systematic and principled manner. Indeed, the last decade has witnessed a surge in the systematic study of computational algorithms for phase retrieval. In this paper we will review these recent advances from a numerical viewpoint. Contents 1. Introduction 2 1.1. Overview 4 2. Phase retrieval and ptychography: basic setup 5 2.1. Mathematical formulation 5 2.2. Prior information 6 2.3. Measurement techniques 7 2.4. Measurement of coded diffraction patterns 8 2.5. Ptychography 10 2.6. Ptychography and time-frequency analysis 11 2.7. 2D Ptychography 12 3. Uniqueness, ambiguities, noise 13 3.1. Uniqueness and ambiguities with coded diffraction patterns 14 3.2. Ambiguities with one diffraction pattern 15 3.3. Phase retrieval as feasibility 17 3.4. Noise models and log-likelihood functions 18 3.5. Spectral gap and local convexity 20 4. Nonconvex optimization 20 4.1. Alternating Projections (AP) 20 4.2. Averaged Alternating Reflections (AAR) 21 4.3.
    [Show full text]
  • Algorithms for Coherent Diffractive Imaging with X-Ray Lasers
    Digital Comprehensive Summaries of Uppsala Dissertations from the Faculty of Science and Technology 1589 Algorithms for Coherent Diffractive Imaging with X-ray Lasers BENEDIKT J. DAURER ACTA UNIVERSITATIS UPSALIENSIS ISSN 1651-6214 ISBN 978-91-513-0129-7 UPPSALA urn:nbn:se:uu:diva-329012 2017 Dissertation presented at Uppsala University to be publicly examined in Room B7:101a, Biomedicinska Centrum (BMC), Husargatan 3, Uppsala, Friday, 15 December 2017 at 13:00 for the degree of Doctor of Philosophy. The examination will be conducted in English. Faculty examiner: Professor Richard Neutze (University of Gothenburg). Abstract Daurer, B. J. 2017. Algorithms for Coherent Diffractive Imaging with X-ray Lasers. Digital Comprehensive Summaries of Uppsala Dissertations from the Faculty of Science and Technology 1589. 64 pp. Uppsala: Acta Universitatis Upsaliensis. ISBN 978-91-513-0129-7. Coherent diffractive imaging (CDI) has become a very popular technique over the past two decades. CDI is a "lensless" imaging method which replaces the objective lens of a conventional microscope by a computational image reconstruction procedure. Its increase in popularity came together with the development of X-ray free-electron lasers (XFELs) which produce extremely bright and coherent X-rays. By facilitating these unique properties, CDI enables structure determination of non-crystalline samples at nanometre resolution and has many applications in structural biology, material science and X-ray optics among others. This work focuses on two specific CDI techniques, flash X-ray diffractive imaging (FXI) on biological samples and X- ray ptychography. While the first FXI demonstrations using soft X-rays have been quite promising, they also revealed remaining technical challenges.
    [Show full text]
  • Principles of Different X-Ray Phase-Contrast Imaging: a Review
    applied sciences Review Principles of Different X-ray Phase-Contrast Imaging: A Review Siwei Tao 1,†, Congxiao He 1,†, Xiang Hao 1, Cuifang Kuang 1,2,* and Xu Liu 1,2,* 1 State Key Laboratory of Modern Optical Instrumentation, College of Optical Science and Engineering, Zhejiang University, Hangzhou 310027, China; [email protected] (S.T.); [email protected] (C.H.); [email protected] (X.H.) 2 Collaborative Innovation Center of Extreme Optics, Shanxi University, Taiyuan 030006, China * Correspondence: [email protected] (C.K.); [email protected] (X.L.) † These authors contributed equally to this work and should be considered co-first authors. Abstract: Numerous advances have been made in X-ray technology in recent years. X-ray imag- ing plays an important role in the nondestructive exploration of the internal structures of objects. However, the contrast of X-ray absorption images remains low, especially for materials with low atomic numbers, such as biological samples. X-ray phase-contrast images have an intrinsically higher contrast than absorption images. In this review, the principles, milestones, and recent progress of X-ray phase-contrast imaging methods are demonstrated. In addition, prospective applications are presented. Keywords: X-ray imaging; phase retrieval 1. Introduction As discovered by Wilhelm Conrad Röntgen, X-rays are electromagnetic waves with −12 −8 wavelengths ranging from approximately 10 to 10 m. The X-ray source, which is usually called an X-ray tube, is a vacuum chamber containing the anode and the cathode. Citation: Tao, S.; He, C.; Hao, X.; When a high current is applied to the cathode, its temperature increases, so electrons Kuang, C.; Liu, X.
    [Show full text]
  • Phase Retrieval with Application to Optical Imaging
    1 Phase Retrieval with Application to Optical Imaging Yoav Shechtman∗y, Yonina C. Eldarz, Oren Cohen∗, Henry N. Chapmanx{k, Jianwei Miao∗∗ and Mordechai Segev∗ ∗Department of Physics Technion, Israel Institute of Technology, Israel 32000 yDepartment of Chemistry, Stanford University, Stanford, California 94305, USA zDepartment of Electrical Engineering, Technion, Israel Institute of Technology, Israel 32000 xCenter for Free-Electron Laser Science, DESY, Notkestrasse 85, 22607 Hamburg, Germany {University of Hamburg, Luruper Chaussee 149, 22761 Hamburg, Germany kCenter for Ultrafast Imaging, 22607 Hamburg, Germany ∗∗Department of Physics and Astronomy, and California NanoSystems Institute, University of California, Los Angeles, CA 90095, USA Email: [email protected] I. INTRODUCTION a known quadratic phase factor. Thus, measuring the far- field, magnitude and phase, would facilitate recovery of the The problem of phase retrieval, namely – the recovery of a optical image (the wavefield). However, as noted above, the function given the magnitude of its Fourier transform - arises optical phase cannot be measured directly by an electronic in various fields of science and engineering, including electron detector. Here is where algorithmic phase retrieval comes into microscopy, crystallography, astronomy, and optical imaging. play, offering a means for recovering the phase given the Exploring phase retrieval in optical settings, specifically when measurement of the magnitude of the optical far-field and the light originates from a laser, is natural, because optical some prior knowledge. detection devices (e.g., ccd cameras, photosensitive films, the human eye) cannot measure the phase of a light wave. This is because, generally, optical measurement devices that rely on converting photons to electrons (current) do not allow direct The purpose of this review article is to provide a con- recording of the phase: the electromagnetic field oscillates at temporary review of phase retrieval in optical imaging.
    [Show full text]
  • Phase Retrieval Using Conditional Generative Adversarial Networks
    Phase Retrieval Using Conditional Generative Adversarial Networks Tobias Uelwer, Alexander Oberstraß and Stefan Harmeling Department of Computer Science Heinrich Heine University Düsseldorf Düsseldorf, Germany Email: {tobias.uelwer, alexander.oberstrass, stefan.harmeling}@hhu.de Abstract—In this paper, we propose the application of con- C. Prior Work ditional generative adversarial networks to solve various phase In practice, traditional projection-based methods like the retrieval problems. We show that including knowledge of the measurement process at training time leads to an optimization Gerchberg-Saxton algorithm [5], the hybrid input-output at test time that is more robust to initialization than existing (HIO) algorithm [6] or the relaxed averaged alternating re- approaches involving generative models. In addition, conditioning flections (RAAR) algorithm [7] require the magnitudes of the the generator network on the measurements enables us to achieve Fourier measurements to be oversampled [8], as demonstrated much more detailed results. We empirically demonstrate that in Figure 1. The influence of oversampling on the Fourier these advantages provide meaningful solutions to the Fourier and the compressive phase retrieval problem and that our method phase retrieval problem is discussed in [9]. Without over- outperforms well-established projection-based methods as well as sampling more prior knowledge about the signal is needed. existing methods that are based on neural networks. Like other Traditional methods, however, merely take some handcrafted deep learning methods, our approach is robust to noise and can prior information like signal sparsity into the reconstruction therefore be useful for real-world applications. process. Sparse phase retrieval has been discussed in [10], [11], [12], [13].
    [Show full text]
  • Practical Phase Retrieval: Low-Photon Holography
    Under review as a conference paper at ICLR 2021 PRACTICAL PHASE RETRIEVAL:LOW-PHOTON HOLOGRAPHY WITH UNTRAINED PRIORS Anonymous authors Paper under double-blind review ABSTRACT Phase retrieval is the inverse problem of recovering a signal from magnitude-only Fourier measurements, and underlies numerous imaging modalities, such as Co- herent Diffraction Imaging (CDI). A variant of this setup, known as holography, includes a reference object that is placed adjacent to the specimen of interest be- fore measurements are collected. The resulting inverse problem, known as holo- graphic phase retrieval, is well-known to have improved problem conditioning relative to the original. This innovation, i.e. Holographic CDI, becomes crucial at the nanoscale, where imaging specimens such as viruses, proteins, and crys- tals require low-photon measurements. This data is highly corrupted by Poisson shot noise, and often lacks low-frequency content as well. In this work, we in- troduce a dataset-free deep learning framework for holographic phase retrieval adapted to these challenges. The key ingredients of our approach are the explicit and flexible incorporation of the physical forward model into an automatic differ- entiation procedure, the Poisson log-likelihood objective function, and an optional untrained deep image prior. We perform extensive evaluation under realistic con- ditions. Compared to competing classical methods, our method recovers signal from higher noise levels and is more resilient to suboptimal reference design, as well as to large missing regions of low frequencies in the observations. To the best of our knowledge, this is the first work to consider a dataset-free machine learning approach for holographic phase retrieval.
    [Show full text]
  • Phase Retrieval Under a Generative Prior
    Phase Retrieval Under a Generative Prior Paul Hand⇤ Oscar Leong Northeastern University Rice University [email protected] [email protected] Vladislav Voroninski Helm.ai [email protected] Abstract We introduce a novel deep learning inspired formulation of the phase retrieval n problem, which asks to recover a signal y0 R from m quadratic observations, under structural assumptions on the underlying2 signal. As is common in many imaging problems, previous methodologies have considered natural signals as being sparse with respect to a known basis, resulting in the decision to enforce a generic sparsity prior. However, these methods for phase retrieval have encountered possibly fundamental limitations, as no computationally efficient algorithm for sparse phase retrieval has been proven to succeed with fewer than O(k2 log n) generic measurements, which is larger than the theoretical optimum of O(k log n). In this paper, we propose a new framework for phase retrieval by modeling natural signals as being in the range of a deep generative neural network G : Rk Rn. We introduce an empirical risk formulation that has favorable global geometry! for gradient methods, as soon as m = O(kd2 log n), under the model of a d-layer fully-connected neural network with random weights. Specifically, when suitable deterministic conditions on the generator and measurement matrix are met, we construct a descent direction for any point outside of a small neighborhood around the true k-dimensional latent code and a negative multiple thereof. This formulation for structured phase retrieval thus benefits from two effects: generative priors can more tightly represent natural signals than sparsity priors, and this empirical risk formulation can exploit those generative priors at an information theoretically optimal sample complexity, unlike for a sparsity prior.
    [Show full text]
  • Resolution Enhancement in Coherent Diffraction Imaging Using High Dynamic Range Image
    hv photonics Communication Resolution Enhancement in Coherent Diffraction Imaging Using High Dynamic Range Image Yuanyuan Liu , Qingwen Liu * , Shuangxiang Zhao, Wenchen Sun, Bingxin Xu and Zuyuan He State Key Laboratory of Advanced Optical Communication Systems and Networks, Shanghai Jiao Tong University, Shanghai 200240, China; [email protected] (Y.L.); [email protected] (S.Z.); [email protected] (W.S.); [email protected] (B.X.); [email protected] (Z.H.) * Correspondence: [email protected] Abstract: In a coherent diffraction imaging (CDI) system, the information of the sample is retrieved from the diffraction patterns recorded by the image sensor via multiple iterations. The limited dynamic range of the image sensor restricts the resolution of the reconstructed sample information. To alleviate this problem, the high dynamic range imaging technology is adopted to increase the signal-to-noise ratio of the diffraction patterns. A sequence of raw diffraction images with differently exposure time are recorded by the image sensor. Then, they are fused to generate a high quality diffraction pattern based on the response function of the image sensor. With the fused diffraction pat- terns, the resolution of the coherent diffraction imaging can be effectively improved. The experiments on USAF resolution card is carried out to verify the effectiveness of our proposed method, in which the spatial resolution is improved by 1.8 times using the high dynamic range imaging technology. Keywords: coherent diffraction imaging; high dynamic range imaging; super resolution; multi-wavelength imaging system Citation: Liu, Y.; Liu, Q.; Zhao, S.; Sun, W.; Xu, B.; He, Z.
    [Show full text]