Analysis and Design of Oversampled Digital-To-Analog Converters
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Design of Optimal Feedback Filters with Guaranteed Closed-Loop Stability for Oversampled Noise-Shaping Subband Quantizers
49th IEEE Conference on Decision and Control December 15-17, 2010 Hilton Atlanta Hotel, Atlanta, GA, USA Design of Optimal Feedback Filters with Guaranteed Closed-Loop Stability for Oversampled Noise-Shaping Subband Quantizers SanderWahls HolgerBoche. Abstract—We consider the oversampled noise-shaping sub- T T T T ] ] ] ] band quantizer (ONSQ) with the quantization noise being q q v q,q v q,q + Quant- + + + + modeled as white noise. The problem at hand is to design an q - q izer q q - q q ,...,w ,...,w optimal feedback filter. Optimal feedback filters with regard 1 1 ,...,v ,...,v to the current standard model of the ONSQ inhabit several + q,1 q,1 w=[w + w=[w =[v =[v shortcomings: the stability of the feedback loop is not ensured - q q v v and the noise is considered independent of both the input and u ŋ u ŋ -1 -1 the feedback filter. Another previously unknown disadvantage, q z F(z) q q z F(z) q which we prove in our paper, is that optimal feedback filters in the standard model are never unique. The goal of this paper is (a) Real model: η is the qnt. error (b) Linearized model: η is white noise to show how these shortcomings can be overcome. The stability issue is addressed by showing that every feedback filter can be Figure 1: Noise-Shaping Quantizer “stabilized” in the sense that we can find another feedback filter which stabilizes the feedback loop and achieves a performance w v E (z) p 1 q,1 p R (z) equal (or arbitrarily close) to the original filter. -
Designing Commutative Cascades of Multidimensional Upsamplers And
IEEE SIGNAL PROCESSING LETTERS: SPL.SP.4.1 THEORY, ALGORITHMS, AND SYSTEMS 0 Designing Commutative Cascades of Multidimensional Upsamplers and Downsamplers Brian L. Evans, Member, IEEE Abstract In multiple dimensions, the cascade of an upsampler by L and a downsampler by L commutes if and only if the integer matrices L and M are right coprime and LM = ML. This pap er presents algorithms to design L and M that yield commutative upsampler/dowsampler cascades. We prove that commutativity is p ossible if the 1 Jordan canonical form of the rational resampling matrix R = LM is equivalent to the Smith-McMillan form of R. A necessary condition for this equivalence is that R has an eigendecomp osition and the eigenvalues are rational. B. L. Evans is with the Department of Electrical and Computer Engineering, The UniversityofTexas at Austin, Austin, TX 78712-1084, USA. E-mail: [email protected], Web: http://www.ece.utexas.edu/~b evans, Phone: 512 232-1457, Fax: 512 471-5907. This work was sp onsored in part by NSF CAREER Award under Grant MIP-9702707. July 31, 1997 DRAFT IEEE SIGNAL PROCESSING LETTERS: SPL.SP.4.1 THEORY, ALGORITHMS, AND SYSTEMS 1 I. Introduction 1 Resampling systems scale the sampling rate by a rational factor R = L=M = LM , or 1 equivalently decimate by H = M=L = L M [1], by essentially upsampling by L, ltering, and downsampling by M . In converting compact disc data sampled at 44.1 kHz to digital audio tap e 48000 Hz 160 data sampled at 48 kHz, R = = . Because we can always factor R into coprime 44100 Hz 147 integers L and M , we can always commute the upsampler and downsampler which leads to ecient p olyphase structures of the resampling system. -
ESE 531: Digital Signal Processing
ESE 531: Digital Signal Processing Lec 12: February 21st, 2017 Data Converters, Noise Shaping (con’t) Penn ESE 531 Spring 2017 - Khanna Lecture Outline ! Data Converters " Anti-aliasing " ADC " Quantization " Practical DAC ! Noise Shaping Penn ESE 531 Spring 2017 - Khanna 2 ADC Penn ESE 531 Spring 2017 - Khanna 3 Anti-Aliasing Filter with ADC Penn ESE 531 Spring 2017 - Khanna 4 Oversampled ADC Penn ESE 531 Spring 2017 - Khanna 5 Oversampled ADC Penn ESE 531 Spring 2017 - Khanna 6 Oversampled ADC Penn ESE 531 Spring 2017 - Khanna 7 Oversampled ADC Penn ESE 531 Spring 2017 - Khanna 8 Sampling and Quantization Penn ESE 531 Spring 2017 - Khanna 9 Sampling and Quantization Penn ESE 531 Spring 2017 - Khanna 10 Effect of Quantization Error on Signal ! Quantization error is a deterministic function of the signal " Consequently, the effect of quantization strongly depends on the signal itself ! Unless, we consider fairly trivial signals, a deterministic analysis is usually impractical " More common to look at errors from a statistical perspective " "Quantization noise” ! Two aspects " How much noise power (variance) does quantization add to our samples? " How is this noise distributed in frequency? Penn ESE 531 Spring 2017 - Khanna 11 Quantization Error ! Model quantization error as noise ! In that case: Penn ESE 531 Spring 2017 - Khanna 12 Ideal Quantizer ! Quantization step Δ ! Quantization error has sawtooth shape, ! Bounded by –Δ/2, +Δ/2 ! Ideally infinite input range and infinite number of quantization levels Penn ESE 568 Fall 2016 - Khanna adapted from Murmann EE315B, Stanford 13 Ideal B-bit Quantizer ! Practical quantizers have a limited input range and a finite set of output codes ! E.g. -
A Subjective Evaluation of Noise-Shaping Quantization for Adaptive
332 IEEE TRANSACTIONS ON COMMUNICATIONS, VOL. 36, NO. 3, MARCH 1988 A Subjective Evaluation of Noise-S haping Quantization for Adaptive Intra-/Interframe DPCM Coding of Color Television Signals BERND GIROD, H AKAN ALMER, LEIF BENGTSSON, BJORN CHRISTENSSON, AND PETER WEISS Abstract-Nonuniform quantizers for just not visible reconstruction quantizers for just not visible eri-ors have been presented in errors in an adaptive intra-/interframe DPCM scheme for component- [12]-[I41 for the luminance and in [IS], [I61 for the color coded color television signals are presented, both for conventional DPCM difference signals. An investigation concerning the visibility and for noise-shaping DPCM. Noise feedback filters that minimize the of quantization errors for an adaiptive intra-/interframe lumi- visibility of reconstruction errors by spectral shaping are designed for Y, nance DPCM coder has been reported by Westerkamp [17]. R-Y, and B-Y. A closed-form description of the “masking function” is In this paper, we present quantization characteristics for the derived which leads to the one-parameter “6 quantizer” characteristic. luminance and the color dilference signals that lead to just not Subjective tests that were carried out to determine visibility thresholds for visible reconstruction errors in sin adaptive intra-/interframe reconstruction errors for conventional DPCM and for noise shaping DPCM scheme. These quantizers have been determined by DPCM show significant gains by noise shaping. For a transmission rate means of subjective tests. In order to evaluate the improve- of around 30 Mbitsls, reconstruction errors are almost always below the ments that can be achieved by reconstruction noise shaping visibility threshold if variable length encoding of the prediction error is [l 11, we compare the quantization characteristics for just not combined with noise shaping within a 3:l:l system. -
Quantization Noise Shaping on Arbitrary Frame Expansions
Hindawi Publishing Corporation EURASIP Journal on Applied Signal Processing Volume 2006, Article ID 53807, Pages 1–12 DOI 10.1155/ASP/2006/53807 Quantization Noise Shaping on Arbitrary Frame Expansions Petros T. Boufounos and Alan V. Oppenheim Digital Signal Processing Group, Massachusetts Institute of Technology, 77 Massachusetts Avenue, Room 36-615, Cambridge, MA 02139, USA Received 2 October 2004; Revised 10 June 2005; Accepted 12 July 2005 Quantization noise shaping is commonly used in oversampled A/D and D/A converters with uniform sampling. This paper consid- ers quantization noise shaping for arbitrary finite frame expansions based on generalizing the view of first-order classical oversam- pled noise shaping as a compensation of the quantization error through projections. Two levels of generalization are developed, one a special case of the other, and two different cost models are proposed to evaluate the quantizer structures. Within our framework, the synthesis frame vectors are assumed given, and the computational complexity is in the initial determination of frame vector ordering, carried out off-line as part of the quantizer design. We consider the extension of the results to infinite shift-invariant frames and consider in particular filtering and oversampled filter banks. Copyright © 2006 P. T. Boufounos and A. V. Oppenheim. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. 1. INTRODUCTION coefficient through a projection onto the space defined by another synthesis frame vector. This requires only knowl- Quantization methods for frame expansions have received edge of the synthesis frame set and a prespecified order- considerable attention in the last few years. -
Color Error Diffusion with Generalized Optimum Noise
COLOR ERROR DIFFUSION WITH GENERALIZED OPTIMUM NOISE SHAPING Niranjan Damera-Venkata Brian L. Evans Halftoning and Image Pro cessing Group Emb edded Signal Pro cessing Lab oratory Hewlett-Packard Lab oratories Dept. of Electrical and Computer Engineering 1501 Page Mill Road The University of Texas at Austin Palo Alto, CA 94304 Austin, TX 78712-1084 E-mail: [email protected] E-mail: [email protected] In this pap er, we derive the optimum matrix-valued er- ABSTRACT ror lter using the matrix gain mo del [3 ] to mo del the noise We optimize the noise shaping b ehavior of color error dif- shaping b ehavior of color error di usion and a generalized fusion by designing an optimized error lter based on a linear spatially-invariant mo del not necessarily separable prop osed noise shaping mo del for color error di usion and for the human color vision. We also incorp orate the con- a generalized linear spatially-invariant mo del of the hu- straint that all of the RGB quantization error b e di used. man visual system. Our approach allows the error lter We show that the optimum error lter may be obtained to have matrix-valued co ecients and di use quantization as a solution to a matrix version of the Yule-Walker equa- error across channels in an opp onent color representation. tions. A gradient descent algorithm is prop osed to solve the Thus, the noise is shap ed into frequency regions of reduced generalized Yule-Walker equations. In the sp ecial case that human color sensitivity. -
Noise Shaping
INF4420 ΔΣ data converters Spring 2012 Jørgen Andreas Michaelsen ([email protected]) Outline Oversampling Noise shaping Circuit design issues Higher order noise shaping Introduction So far we have considered so called Nyquist data converters. Quantization noise is a fundamental limit. Improving the resolution of the converter, translates to increasing the number of quantization steps (bits). Requires better -1 N+1 component matching, AOL > β 2 , and N+1 -1 -1 GBW > fs ln 2 π β . Introduction ΔΣ modulator based data converters relies on oversampling and noise shaping to improve the resolution. Oversampling means that the data rate is increased to several times what is required by the Nyquist sampling theorem. Noise shaping means that the quantization noise is moved away from the signal band that we are interested in. Introduction We can make a high resolution data converter with few quantization steps! The most obvious trade-off is the increase in speed and more complex digital processing. However, this is a good fit for CMOS. We can apply this to both DACs and ADCs. Oversampling The total quantization noise depends only on the number of steps. Not the bandwidth. If we increase the sampling rate, the quantization noise will not increase and it will spread over a larger area. The power spectral density will decrease. Oversampling Take a regular ADC and run it at a much higher speed than twice the Nyquist frequency. Quantization noise is reduced because only a fraction remains in the signal bandwidth, fb. Oversampling Doubling the OSR improves SNR by 0.5 bit Increasing the resolution by oversampling is not practical. -
Deep Image Prior for Undersampling High-Speed Photoacoustic Microscopy
Photoacoustics 22 (2021) 100266 Contents lists available at ScienceDirect Photoacoustics journal homepage: www.elsevier.com/locate/pacs Deep image prior for undersampling high-speed photoacoustic microscopy Tri Vu a,*, Anthony DiSpirito III a, Daiwei Li a, Zixuan Wang c, Xiaoyi Zhu a, Maomao Chen a, Laiming Jiang d, Dong Zhang b, Jianwen Luo b, Yu Shrike Zhang c, Qifa Zhou d, Roarke Horstmeyer e, Junjie Yao a a Photoacoustic Imaging Lab, Duke University, Durham, NC, 27708, USA b Department of Biomedical Engineering, Tsinghua University, Beijing, 100084, China c Division of Engineering in Medicine, Department of Medicine, Brigham and Women’s Hospital, Harvard Medical School, Cambridge, MA, 02139, USA d Department of Biomedical Engineering and USC Roski Eye Institute, University of Southern California, Los Angeles, CA, 90089, USA e Computational Optics Lab, Duke University, Durham, NC, 27708, USA ARTICLE INFO ABSTRACT Keywords: Photoacoustic microscopy (PAM) is an emerging imaging method combining light and sound. However, limited Convolutional neural network by the laser’s repetition rate, state-of-the-art high-speed PAM technology often sacrificesspatial sampling density Deep image prior (i.e., undersampling) for increased imaging speed over a large field-of-view. Deep learning (DL) methods have Deep learning recently been used to improve sparsely sampled PAM images; however, these methods often require time- High-speed imaging consuming pre-training and large training dataset with ground truth. Here, we propose the use of deep image Photoacoustic microscopy Raster scanning prior (DIP) to improve the image quality of undersampled PAM images. Unlike other DL approaches, DIP requires Undersampling neither pre-training nor fully-sampled ground truth, enabling its flexible and fast implementation on various imaging targets. -
ELEG 5173L Digital Signal Processing Ch. 3 Discrete-Time Fourier Transform
Department of Electrical Engineering University of Arkansas ELEG 5173L Digital Signal Processing Ch. 3 Discrete-Time Fourier Transform Dr. Jingxian Wu [email protected] 2 OUTLINE • The Discrete-Time Fourier Transform (DTFT) • Properties • DTFT of Sampled Signals • Upsampling and downsampling 3 DTFT • Discrete-time Fourier Transform (DTFT) X () x(n)e jn n – (radians): digital frequency • Review: Z-transform: X (z) x(n)zn n0 j X () X (z) | j – Replace z with e . ze • Review: Fourier transform: X () x(t)e jt – (rads/sec): analog frequency 4 DTFT • Relationship between DTFT and Fourier Transform – Sample a continuous time signal x a ( t ) with a sampling period T xs (t) xa (t) (t nT ) xa (nT ) (t nT ) n n – The Fourier Transform of ys (t) jt jnT X s () xs (t)e dt xa (nT)e n – Define: T • : digital frequency (unit: radians) • : analog frequency (unit: radians/sec) – Let x(n) xa (nT) X () X s T 5 DTFT • Relationship between DTFT and Fourier Transform (Cont’d) – The DTFT can be considered as the scaled version of the Fourier transform of the sampled continuous-time signal jt jnT X s () xs (t)e dt xa (nT)e n x(n) x (nT) T a jn X () X s x(n)e T n 6 DTFT • Discrete Frequency – Unit: radians (the unit of continuous frequency is radians/sec) – X ( ) is a periodic function with period 2 j2 n jn j2n jn X ( 2 ) x(n)e x(n)e e x(n)e X () n n n – We only need to consider for • For Fourier transform, we need to consider 1 – f T 2 2T 1 – f T 2 2T 7 DTFT • Example: find the DTFT of the following signal – 1. -
F • Aliasing Distortion • Quantization Noise • Bandwidth Limitations • Cost of A/D & D/A Conversion
Aliasing • Aliasing distortion • Quantization noise • A 1 Hz Sine wave sampled at 1.8 Hz • Bandwidth limitations • A 0.8 Hz sine wave sampled at 1.8 Hz • Cost of A/D & D/A conversion -fs fs THE UNIVERSITY OF TEXAS AT AUSTIN Advantages of Digital Systems Perfect reconstruction of a Better trade-off between signal is possible even after bandwidth and noise severe distortion immunity performance digital analog bandwidth Increase signal-to-noise ratio simply by adding more bits SNR = -7.2 + 6 dB/bit THE UNIVERSITY OF TEXAS AT AUSTIN Advantages of Digital Systems Programmability • Modifiable in the field • Implement multiple standards • Better user interfaces • Tolerance for changes in specifications • Get better use of hardware for low-speed operations • Debugging • User programmability THE UNIVERSITY OF TEXAS AT AUSTIN Disadvantages of Digital Systems Programmability • Speed is too slow for some applications • High average power and peak power consumption RISC (2 Watts) vs. DSP (50 mW) DATA PROG MEMORY MEMORY HARVARD ARCHITECTURE • Aliasing from undersampling • Clipping from quantization Q[v] v v THE UNIVERSITY OF TEXAS AT AUSTIN Analog-to-Digital Conversion 1 --- T h(t) Q[.] xt() yt() ynT() yˆ()nT Anti-Aliasing Sampler Quantizer Filter xt() y(nT) t n y(t) ^y(nT) t n THE UNIVERSITY OF TEXAS AT AUSTIN Resampling Changing the Sampling Rate • Conversion between audio formats Compact 48.0 Digital Disc ---------- Audio Tape 44.1 KHz44.1 48 KHz • Speech compression Speech 1 Speech for on DAT --- Telephone 48 KHz 6 8 KHz • Video format conversion -
Sonically Optimized Noise Shaping Techniques
Sonically Optimized Noise Shaping Techniques Second edition Alexey Lukin [email protected] 2002 In this article we compare different commercially available noise shaping algo- rithms and introduce a new highly optimized frequency response curve for noise shap- ing filter implemented in our ExtraBit Mastering Processor. Contents INTRODUCTION ......................................................................................................................... 2 TESTED NOISE SHAPERS ......................................................................................................... 2 CRITERIONS OF COMPARISON............................................................................................... 3 RESULTS...................................................................................................................................... 4 NOISE STATISTICS & PERCEIVED LOUDNESS .............................................................................. 4 NOISE SPECTRUMS ..................................................................................................................... 5 No noise shaping (TPDF dithering)..................................................................................... 5 Cool Edit (C1 curve) ............................................................................................................5 Cool Edit (C3 curve) ............................................................................................................6 POW-R (pow-r1 mode)........................................................................................................ -
Clock Jitter Effects on the Performance of ADC Devices
Clock Jitter Effects on the Performance of ADC Devices Roberto J. Vega Luis Geraldo P. Meloni Universidade Estadual de Campinas - UNICAMP Universidade Estadual de Campinas - UNICAMP P.O. Box 05 - 13083-852 P.O. Box 05 - 13083-852 Campinas - SP - Brazil Campinas - SP - Brazil [email protected] [email protected] Karlo G. Lenzi Centro de Pesquisa e Desenvolvimento em Telecomunicac¸oes˜ - CPqD P.O. Box 05 - 13083-852 Campinas - SP - Brazil [email protected] Abstract— This paper aims to demonstrate the effect of jitter power near the full scale of the ADC, the noise power is on the performance of Analog-to-digital converters and how computed by all FFT bins except the DC bin value (it is it degrades the quality of the signal being sampled. If not common to exclude up to 8 bins after the DC zero-bin to carefully controlled, jitter effects on data acquisition may severely impacted the outcome of the sampling process. This analysis avoid any spectral leakage of the DC component). is of great importance for applications that demands a very This measure includes the effect of all types of noise, the good signal to noise ratio, such as high-performance wireless distortion and harmonics introduced by the converter. The rms standards, such as DTV, WiMAX and LTE. error is given by (1), as defined by IEEE standard [5], where Index Terms— ADC Performance, Jitter, Phase Noise, SNR. J is an exact integer multiple of fs=N: I. INTRODUCTION 1 s X = jX(k)j2 (1) With the advance of the technology and the migration of the rms N signal processing from analog to digital, the use of analog-to- k6=0;J;N−J digital converters (ADC) became essential.