Can Compressed Sensing Beat the Nyquist Sampling Rate?
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Compressive Phase Retrieval Lei Tian
Compressive Phase Retrieval by Lei Tian B.S., Tsinghua University (2008) S.M., Massachusetts Institute of Technology (2010) Submitted to the Department of Mechanical Engineering in partial fulfillment of the requirements for the degree of Doctor of Philosophy at the MASSACHUSETTS INSTITUTE OF TECHNOLOGY June 2013 c Massachusetts Institute of Technology 2013. All rights reserved. Author.............................................................. Department of Mechanical Engineering May 18, 2013 Certified by. George Barbastathis Professor Thesis Supervisor Accepted by . David E. Hardt Chairman, Department Committee on Graduate Students 2 Compressive Phase Retrieval by Lei Tian Submitted to the Department of Mechanical Engineering on May 18, 2013, in partial fulfillment of the requirements for the degree of Doctor of Philosophy Abstract Recovering a full description of a wave from limited intensity measurements remains a central problem in optics. Optical waves oscillate too fast for detectors to measure anything but time{averaged intensities. This is unfortunate since the phase can reveal important information about the object. When the light is partially coherent, a complete description of the phase requires knowledge about the statistical correlations for each pair of points in space. Recovery of the correlation function is a much more challenging problem since the number of pairs grows much more rapidly than the number of points. In this thesis, quantitative phase imaging techniques that works for partially co- herent illuminations are investigated. In order to recover the phase information with few measurements, the sparsity in each underly problem and efficient inversion meth- ods are explored under the framework of compressed sensing. In each phase retrieval technique under study, diffraction during spatial propagation is exploited as an ef- fective and convenient mechanism to uniformly distribute the information about the unknown signal into the measurement space. -
Discrete - Time Signals and Systems
Discrete - Time Signals and Systems Sampling – II Sampling theorem & Reconstruction Yogananda Isukapalli Sampling at diffe- -rent rates From these figures, it can be concluded that it is very important to sample the signal adequately to avoid problems in reconstruction, which leads us to Shannon’s sampling theorem 2 Fig:7.1 Claude Shannon: The man who started the digital revolution Shannon arrived at the revolutionary idea of digital representation by sampling the information source at an appropriate rate, and converting the samples to a bit stream Before Shannon, it was commonly believed that the only way of achieving arbitrarily small probability of error in a communication channel was to 1916-2001 reduce the transmission rate to zero. All this changed in 1948 with the publication of “A Mathematical Theory of Communication”—Shannon’s landmark work Shannon’s Sampling theorem A continuous signal xt( ) with frequencies no higher than fmax can be reconstructed exactly from its samples xn[ ]= xn [Ts ], if the samples are taken at a rate ffs ³ 2,max where fTss= 1 This simple theorem is one of the theoretical Pillars of digital communications, control and signal processing Shannon’s Sampling theorem, • States that reconstruction from the samples is possible, but it doesn’t specify any algorithm for reconstruction • It gives a minimum sampling rate that is dependent only on the frequency content of the continuous signal x(t) • The minimum sampling rate of 2fmax is called the “Nyquist rate” Example1: Sampling theorem-Nyquist rate x( t )= 2cos(20p t ), find the Nyquist frequency ? xt( )= 2cos(2p (10) t ) The only frequency in the continuous- time signal is 10 Hz \ fHzmax =10 Nyquist sampling rate Sampling rate, ffsnyq ==2max 20 Hz Continuous-time sinusoid of frequency 10Hz Fig:7.2 Sampled at Nyquist rate, so, the theorem states that 2 samples are enough per period. -
Compressed Digital Holography: from Micro Towards Macro
Compressed digital holography: from micro towards macro Colas Schretter, Stijn Bettens, David Blinder, Beatrice Pesquet-Popescu, Marco Cagnazzo, Frederic Dufaux, Peter Schelkens To cite this version: Colas Schretter, Stijn Bettens, David Blinder, Beatrice Pesquet-Popescu, Marco Cagnazzo, et al.. Compressed digital holography: from micro towards macro. Applications of Digital Image Processing XXXIX, SPIE, Aug 2016, San Diego, United States. hal-01436102 HAL Id: hal-01436102 https://hal.archives-ouvertes.fr/hal-01436102 Submitted on 10 Jan 2020 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Compressed digital holography: from micro towards macro Colas Schrettera,c, Stijn Bettensa,c, David Blindera,c, Béatrice Pesquet-Popescub, Marco Cagnazzob, Frédéric Dufauxb, and Peter Schelkensa,c aDept. of Electronics and Informatics (ETRO), Vrije Universiteit Brussel, Brussels, Belgium bLTCI, CNRS, Télécom ParisTech, Université Paris-Saclay, Paris, France ciMinds, Technologiepark 19, Zwijnaarde, Belgium ABSTRACT The age of computational imaging is merging the physical hardware-driven approach of photonics with advanced signal processing methods from software-driven computer engineering and applied mathematics. The compressed sensing theory in particular established a practical framework for reconstructing the scene content using few linear combinations of complex measurements and a sparse prior for regularizing the solution. -
Compressive Sensing Off the Grid
Compressive sensing off the grid Abstract— We consider the problem of estimating the fre- Indeed, one significant drawback of the discretization quency components of a mixture of s complex sinusoids approach is the performance degradation when the true signal from a random subset of n regularly spaced samples. Unlike is not exactly supported on the grid points, the so called basis previous work in compressive sensing, the frequencies are not assumed to lie on a grid, but can assume any values in the mismatch problem [13], [15], [16]. When basis mismatch normalized frequency domain [0; 1]. We propose an atomic occurs, the true signal cannot be sparsely represented by the norm minimization approach to exactly recover the unobserved assumed dictionary determined by the grid points. One might samples, which is then followed by any linear prediction method attempt to remedy this issue by using a finer discretization. to identify the frequency components. We reformulate the However, increasing the discretization level will also increase atomic norm minimization as an exact semidefinite program. By constructing a dual certificate polynomial using random the coherence of the dictionary. Common wisdom in com- kernels, we show that roughly s log s log n random samples pressive sensing suggests that high coherence would also are sufficient to guarantee the exact frequency estimation with degrade the performance. It remains unclear whether over- high probability, provided the frequencies are well separated. discretization is beneficial to solving the problems. Finer Extensive numerical experiments are performed to illustrate gridding also results in higher computational complexity and the effectiveness of the proposed method. -
The Nyquist Sampling Rate for Spiraling Curves 11
THE NYQUIST SAMPLING RATE FOR SPIRALING CURVES PHILIPPE JAMING, FELIPE NEGREIRA & JOSE´ LUIS ROMERO Abstract. We consider the problem of reconstructing a compactly supported function from samples of its Fourier transform taken along a spiral. We determine the Nyquist sampling rate in terms of the density of the spiral and show that, below this rate, spirals suffer from an approximate form of aliasing. This sets a limit to the amount of under- sampling that compressible signals admit when sampled along spirals. More precisely, we derive a lower bound on the condition number for the reconstruction of functions of bounded variation, and for functions that are sparse in the Haar wavelet basis. 1. Introduction 1.1. The mobile sampling problem. In this article, we consider the reconstruction of a compactly supported function from samples of its Fourier transform taken along certain curves, that we call spiraling. This problem is relevant, for example, in magnetic resonance imaging (MRI), where the anatomy and physiology of a person are captured by moving sensors. The Fourier sampling problem is equivalent to the sampling problem for bandlimited functions - that is, functions whose Fourier transform are supported on a given compact set. The most classical setting concerns functions of one real variable with Fourier transform supported on the unit interval [ 1/2, 1/2], and sampled on a grid ηZ, with η > 0. The sampling rate η determines whether− every bandlimited function can be reconstructed from its samples: reconstruction fails if η > 1 and succeeds if η 6 1 [42]. The transition value η = 1 is known as the Nyquist sampling rate, and it is the benchmark for all sampling schemes: modern sampling strategies that exploit the particular structure of a certain class of signals are praised because they achieve sub-Nyquist sampling rates. -
2.161 Signal Processing: Continuous and Discrete Fall 2008
MIT OpenCourseWare http://ocw.mit.edu 2.161 Signal Processing: Continuous and Discrete Fall 2008 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms. MASSACHUSETTS INSTITUTE OF TECHNOLOGY DEPARTMENT OF MECHANICAL ENGINEERING 2.161 Signal Processing - Continuous and Discrete 1 Sampling and the Discrete Fourier Transform 1 Sampling Consider a continuous function f(t) that is limited in extent, T1 · t < T2. In order to process this function in the computer it must be sampled and represented by a ¯nite set of numbers. The most common sampling scheme is to use a ¯xed sampling interval ¢T and to form a sequence of length N: ffng (n = 0 : : : N ¡ 1), where fn = f(T1 + n¢T ): In subsequent processing the function f(t) is represented by the ¯nite sequence ffng and the sampling interval ¢T . In practice, sampling occurs in the time domain by the use of an analog-digital (A/D) converter. The mathematical operation of sampling (not to be confused with the physics of sampling) is most commonly described as a multiplicative operation, in which f(t) is multiplied by a Dirac comb sampling function s(t; ¢T ), consisting of a set of delayed Dirac delta functions: X1 s(t; ¢T ) = ±(t ¡ n¢T ): (1) n=¡1 ? We denote the sampled waveform f (t) as X1 ? f (t) = s(t; ¢T )f(t) = f(t)±(t ¡ n¢T ) (2) n=¡1 ? as shown in Fig. 1. Note that f (t) is a set of delayed weighted delta functions, and that the waveform must be interpreted in the distribution sense by the strength (or area) of each component impulse. -
Signal Sampling
FYS3240 PC-based instrumentation and microcontrollers Signal sampling Spring 2017 – Lecture #5 Bekkeng, 30.01.2017 Content – Aliasing – Sampling – Analog to Digital Conversion (ADC) – Filtering – Oversampling – Triggering Analog Signal Information Three types of information: • Level • Shape • Frequency Sampling Considerations – An analog signal is continuous – A sampled signal is a series of discrete samples acquired at a specified sampling rate – The faster we sample the more our sampled signal will look like our actual signal Actual Signal – If not sampled fast enough a problem known as aliasing will occur Sampled Signal Aliasing Adequately Sampled SignalSignal Aliased Signal Bandwidth of a filter • The bandwidth B of a filter is defined to be between the -3 dB points Sampling & Nyquist’s Theorem • Nyquist’s sampling theorem: – The sample frequency should be at least twice the highest frequency contained in the signal Δf • Or, more correctly: The sample frequency fs should be at least twice the bandwidth Δf of your signal 0 f • In mathematical terms: fs ≥ 2 *Δf, where Δf = fhigh – flow • However, to accurately represent the shape of the ECG signal signal, or to determine peak maximum and peak locations, a higher sampling rate is required – Typically a sample rate of 10 times the bandwidth of the signal is required. Illustration from wikipedia Sampling Example Aliased Signal 100Hz Sine Wave Sampled at 100Hz Adequately Sampled for Frequency Only (Same # of cycles) 100Hz Sine Wave Sampled at 200Hz Adequately Sampled for Frequency and Shape 100Hz Sine Wave Sampled at 1kHz Hardware Filtering • Filtering – To remove unwanted signals from the signal that you are trying to measure • Analog anti-aliasing low-pass filtering before the A/D converter – To remove all signal frequencies that are higher than the input bandwidth of the device. -
Sparse Penalties in Dynamical System Estimation
1 Sparsity Penalties in Dynamical System Estimation Adam Charles, M. Salman Asif, Justin Romberg, Christopher Rozell School of Electrical and Computer Engineering Georgia Institute of Technology, Atlanta, Georgia 30332-0250 Email: facharles6,sasif,jrom,[email protected] Abstract—In this work we address the problem of state by the following equations: estimation in dynamical systems using recent developments x = f (x ) + ν in compressive sensing and sparse approximation. We n n n−1 n (1) formulate the traditional Kalman filter as a one-step update yn = Gnxn + n optimization procedure which leads us to a more unified N framework, useful for incorporating sparsity constraints. where xn 2 R represents the signal of interest, N N We introduce three combinations of two sparsity conditions fn(·)jR ! R represents the (assumed known) evo- (sparsity in the state and sparsity in the innovations) M lution of the signal from time n − 1 to n, yn 2 R and write recursive optimization programs to estimate the M is a set of linear measurements of xn, n 2 R state for each model. This paper is meant as an overview N of different methods for incorporating sparsity into the is the associated measurement noise, and νn 2 R dynamic model, a presentation of algorithms that unify the is our modeling error for fn(·) (commonly known as support and coefficient estimation, and a demonstration the innovations). In the case where Gn is invertible that these suboptimal schemes can actually show some (N = M and the matrix has full rank), state estimation performance improvements (either in estimation error or at each iteration reduces to a least squares problem. -
Compressed Sensing Applied to Modeshapes Reconstruction Joseph Morlier, Dimitri Bettebghor
Compressed sensing applied to modeshapes reconstruction Joseph Morlier, Dimitri Bettebghor To cite this version: Joseph Morlier, Dimitri Bettebghor. Compressed sensing applied to modeshapes reconstruction. XXX Conference and exposition on structural dynamics (IMAC 2012), Jan 2012, Jacksonville, FL, United States. pp.1-8, 10.1007/978-1-4614-2425-3_1. hal-01852318 HAL Id: hal-01852318 https://hal.archives-ouvertes.fr/hal-01852318 Submitted on 1 Aug 2018 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. OATAO is an open access repository that collects the work of Toulouse researchers and makes it freely available over the web where possible. This is an author-deposited version published in: http://oatao.univ-toulouse.fr/ Eprints ID: 5163 To cite this document: Morlier, Joseph and Bettebghor, Dimitri Compressed sensing applied to modeshapes reconstruction. (2011) In: IMAC XXX Conference and exposition on structural dynamics, 30 Jan – 02 Feb 2012, Jacksonville, USA. Any correspondence concerning this service should be sent to the repository administrator: [email protected] Compressed sensing applied to modeshapes reconstruction Joseph Morlier 1*, Dimitri Bettebghor 2 1 Université de Toulouse, ICA, ISAE DMSM ,10 avenue edouard Belin 31005 Toulouse cedex 4, France 2 Onera DTIM MS2M, 10 avenue Edouard Belin, Toulouse, France * Corresponding author, Email: [email protected], Phone no: + (33) 5 61 33 81 31, Fax no: + (33) 5 61 33 83 30 ABSTRACT Modal analysis classicaly used signals that respect the Shannon/Nyquist theory. -
Kalman Filtered Compressed Sensing
KALMAN FILTERED COMPRESSED SENSING Namrata Vaswani Dept. of ECE, Iowa State University, Ames, IA, [email protected] ABSTRACT that we address is: can we do better than performing CS at each time separately, if (a) the sparsity pattern (support set) of the transform We consider the problem of reconstructing time sequences of spa- coefficients’ vector changes slowly, i.e. every time, none or only a tially sparse signals (with unknown and time-varying sparsity pat- few elements of the support change, and (b) a prior model on the terns) from a limited number of linear “incoherent” measurements, temporal dynamics of its current non-zero elements is available. in real-time. The signals are sparse in some transform domain re- Our solution is motivated by reformulating the above problem ferred to as the sparsity basis. For a single spatial signal, the solu- as causal minimum mean squared error (MMSE) estimation with a tion is provided by Compressed Sensing (CS). The question that we slow time-varying set of dominant basis directions (or equivalently address is, for a sequence of sparse signals, can we do better than the support of the transform vector). If the support is known, the CS, if (a) the sparsity pattern of the signal’s transform coefficients’ MMSE solution is given by the Kalman filter (KF) [9] for this sup- vector changes slowly over time, and (b) a simple prior model on port. But what happens if the support is unknown and time-varying? the temporal dynamics of its current non-zero elements is available. The initial support can be estimated using CS [7]. -
Robust Compressed Sensing Using Generative Models
Robust Compressed Sensing using Generative Models Ajil Jalal ∗ Liu Liu ECE, UT Austin ECE, UT Austin [email protected] [email protected] Alexandros G. Dimakis Constantine Caramanis ECE, UT Austin ECE, UT Austin [email protected] [email protected] Abstract The goal of compressed sensing is to estimate a high dimensional vector from an underdetermined system of noisy linear equations. In analogy to classical compressed sensing, here we assume a generative model as a prior, that is, we assume the vector is represented by a deep generative model G : Rk ! Rn. Classical recovery approaches such as empirical risk minimization (ERM) are guaranteed to succeed when the measurement matrix is sub-Gaussian. However, when the measurement matrix and measurements are heavy-tailed or have outliers, recovery may fail dramatically. In this paper we propose an algorithm inspired by the Median-of-Means (MOM). Our algorithm guarantees recovery for heavy-tailed data, even in the presence of outliers. Theoretically, our results show our novel MOM-based algorithm enjoys the same sample complexity guarantees as ERM under sub-Gaussian assumptions. Our experiments validate both aspects of our claims: other algorithms are indeed fragile and fail under heavy-tailed and/or corrupted data, while our approach exhibits the predicted robustness. 1 Introduction Compressive or compressed sensing is the problem of reconstructing an unknown vector x∗ 2 Rn after observing m < n linear measurements of its entries, possibly with added noise: y = Ax∗ + η; where A 2 Rm×n is called the measurement matrix and η 2 Rm is noise. Even without noise, this is an underdetermined system of linear equations, so recovery is impossible without a structural assumption on the unknown vector x∗. -
An Overview of Compressed Sensing
What is Compressed Sensing? Main Results Construction of Measurement Matrices Some Topics Not Covered An Overview of Compressed sensing M. Vidyasagar FRS Cecil & Ida Green Chair, The University of Texas at Dallas [email protected], www.utdallas.edu/∼m.vidyasagar Distinguished Professor, IIT Hyderabad [email protected] Ba;a;ga;va;tua;l .=+a;ma mUa; a;tRa and Ba;a;ga;va;tua;l Za;a:=+d;a;}ba Memorial Lecture University of Hyderabad, 16 March 2015 M. Vidyasagar FRS Overview of Compressed Sensing What is Compressed Sensing? Main Results Construction of Measurement Matrices Some Topics Not Covered Outline 1 What is Compressed Sensing? 2 Main Results 3 Construction of Measurement Matrices Deterministic Approaches Probabilistic Approaches A Case Study 4 Some Topics Not Covered M. Vidyasagar FRS Overview of Compressed Sensing What is Compressed Sensing? Main Results Construction of Measurement Matrices Some Topics Not Covered Outline 1 What is Compressed Sensing? 2 Main Results 3 Construction of Measurement Matrices Deterministic Approaches Probabilistic Approaches A Case Study 4 Some Topics Not Covered M. Vidyasagar FRS Overview of Compressed Sensing What is Compressed Sensing? Main Results Construction of Measurement Matrices Some Topics Not Covered Compressed Sensing: Basic Problem Formulation n Suppose x 2 R is known to be k-sparse, where k n. That is, jsupp(x)j ≤ k n, where supp denotes the support of a vector. However, it is not known which k components are nonzero. Can we recover x exactly by taking m n linear measurements of x? M. Vidyasagar FRS Overview of Compressed Sensing What is Compressed Sensing? Main Results Construction of Measurement Matrices Some Topics Not Covered Precise Problem Statement: Basic Define the set of k-sparse vectors n Σk = fx 2 R : jsupp(x)j ≤ kg: m×n Do there exist an integer m, a \measurement matrix" A 2 R , m n and a \demodulation map" ∆ : R ! R , such that ∆(Ax) = x; 8x 2 Σk? Note: Measurements are linear but demodulation map could be nonlinear.