Intermodulation Distortion Modelling and Measurement Techniques for Gan HEMT Characterization

Total Page:16

File Type:pdf, Size:1020Kb

Intermodulation Distortion Modelling and Measurement Techniques for Gan HEMT Characterization Srinidhi Embar Ramanujam Intermodulation Distortion Modelling and Measurement Techniques for GaN HEMT Characterization kassel university press This work has been accepted by the faculty of Electrical Engineering and Computer Science of the University of Kassel as a thesis for acquiring the academic degree of Doktor der Ingenieurwissenschaften (Dr.-Ing.). Supervisers: Prof. Dr.-Ing. G. Kompa Prof. Dr.-Ing. A. Bangert Defense day: 09th December 2008 Bibliographic information published by Deutsche Nationalbibliothek The Deutsche Nationalbibliothek lists this publication in the Deutsche Nationalbibliografie; detailed bibliographic data is available in the Internet at http://dnb.d-nb.de. Zugl.: Kassel, Univ., Diss. 2008 ISBN print: 978-3-89958-654-1 ISBN online: 978-3-89958-655-8 URN: urn:nbn:de:0002-6558 © 2009, kassel university press GmbH, Kassel www.upress.uni-kassel.de Printed by: Unidruckerei, University of Kassel Printed in Germany To my parents and my family for their devotion and prayers Acknowledgements I wish to express my deep gratitude to Prof. Dr.-Ing. G. Kompa who supervised and nurtured me in becoming a researcher. His invaluable support and encouragement gave me confidence in overcoming difficult times. My sincere thanks to Prof. Dr.-Ing. A. Bangert for accepting the task of being my second examiner. Further, I wish to thank Prof. Dr. sc. techn. B. Witzigmann and PD Dr.-Ing. R. Marklein for accepting to be members of the disputation committee. I am thankful to all the members of the department of High Frequency Engineering for their constant support. I wish to express my gratitude to Mrs. H. Nauditt, Dipl.-Ing. J. Weide, Dr. -Ing. A. Z. Markos, Mr. R. Ma, Dipl.-Ing. B. Wittwer, Mr. S. Dahmani, Mr. A. Zamudio, Mr. S. Monsi, and Mr. A. A. Hussein. My sincere thanks to my parents, family members, and friends who are not mentioned by name for their unreserved encouragement and strong support over past several years. This acknowledgement will most certainly be incomplete without thanking the German Research Foundation (DFG) and the European project TARGET (Top Amplifier Research Group in a European Team) for their financial support. Srinidhi Embar Ramanujam Kassel, December 2008 iii Contents 1. Introduction 1 1.1 Research Objectives …………………………………………. 4 2. Nonlinearity and Memory-Effect Characterization 9 2.1 Nonlinear RF Characterization Techniques …………………. 11 2.1.1 Single-Tone Excitation …..…………………………… 11 2.1.2 Two-Tone Excitation ………………………………… 12 2.1.3 Multi-Tone and Spread-Spectra Excitation ……………. 15 2.2 Memory Properties of a Nonlinear System .……………….… 19 2.3 Memory-Effect Manifestation …………………………….… 23 3. Volterra Model of AlGaN/GaN HEMT 28 3.1 Small-Signal Distortion Analysis ……………………….……. 29 3.1.1 Power Series Characterized Memoryless System Analysis 30 3.1.2 Volterra Series Characterized Dynamic System Analysis ... 32 3.1.2.1 Nonlinear Current Method …………………… 33 3.2 Quasi-Linear Small-Signal FET Equivalent Circuit Model …… 40 3.2.1 Taylor Series Coefficient Extraction ..………………… 42 3.2.1.1 Modelling Conductance Nonlinearity .…..….… 42 3.2.1.2 Modelling Capacitance Nonlinearity .………..… 47 3.3 IMD Modelling ……………………………………………… 49 st 3.3.1 1 -order Volterra Kernel ……………………………… 50 nd 3.3.2 2 -order Volterra Kernel ……………………………… 51 rd 3.3.3 3 -order Volterra Kernel .……..………………………. 58 3.3.4 Model Verification ....………………………………… 61 3.4 IMD Vectorial Analysis …..…………………………………. 61 v 3.5 AlGaN/GaN HEMT Linearity Optimisation ………..…………… 63 3.5.1 Gate Field-Plate Based IMD Minimization ………………… 64 3.6 5th-Degree Extension of Volterra Model ………..………………… 66 4. Large-Signal Measurement Technique 71 4.1 Fundamental System Requirements ……………………………… 72 4.1.1 System Description ……….……………………………… 75 4.1.2 System Calibration ………..………………………………. 77 4.2 Termination Properties for IMD Characterization ………...……… 82 4.3 RF Bias Network - Design Guidelines …………...……………….. 85 4.3.1 Characterization Testbench - Baseband and RF Perspective .. 87 4.3.2 Key Design Challenges ….………………..……………… 100 4.4 Broadband Bias Tee Evaluation ………………………………… 111 4.4.1 Memory-Effect Characterization ………..………………… 111 4.4.2 Load-Pull Characterization ………..……………………… 118 4.5 Drain Bias Sensing ……………………………………………… 123 5. IMD Sweet-Spots 130 5.1 Origin …………………………………………………………… 131 5.1.1 Small-Signal IMD Sweet-Spot ………..…………………… 132 5.1.2 Large-Signal IMD Sweet-Spot ..…………………………… 133 5.2 Bias and Load Termination ……………………………………… 138 5.3 Sweet-Spot Reproducibility ……………………………………….. 143 5.3.1 Statistical Process Consistency Evaluation ………………… 143 5.3.2 Experimental Characterization of Large-Signal IMD Sweet-Spots ………………………………………………. 145 5.3.2.1 Two-Tone Stimuli ………………………………… 145 5.3.2.2 Multi-Carrier W-CDMA Stimuli …………..……… 148 vi 6. Conclusion and Future Work 154 Appendices 162 A. FET Based IMD3 Phasors …..……………………………… 162 B. Measurement Accuracy Enhancement Criteria ..……………… 170 C. Pitfalls in Characterizing Device Inherent IMD Behaviour …… 172 D. Correlation Between IMR and ACPR Characteristics ………… 176 References 181 Publications of the Author 191 vii List of Abbreviations 3GPP third generation partnership project ACPR adjacent channel power ratio ADC analog-to-digital converter AM-AM input amplitude modulation to output amplitude modulation conversion AM-PM input amplitude modulation to output phase modulation conversion ANN artificial neural network CAD computer aided design CCDF complementary cumulative distribution function CW continuous wave DiVA dynamic I(V) analyser DMI drain modulation index DPCH dedicated physical channel DUT device under test EVM error vector magnitude FDD frequency division duplex FP field-plate GaAs gallium arsenide GaN gallium nitride GSM global system for mobile communication HEMT high electron mobility transistor MLP multi-level perceptron IF intermediate frequency IMD intermodulation distortion IM3L 3rd-order lower intermodulation distortion IMR intermodulation ratio IP3 3rd-order intercept point LDMOS laterally diffused metal oxide semiconductor LTE long term evolution MESFET metal semiconductor field effect transistor MTA microwave transition analyser OFDM orthogonal frequency division multiplexing PA power amplifier PAE power added efficiency PAR peak-to-average ratio QPSK quadrature phase shift keying RF radio frequency UMTS universal mobile telecommunications system VNA vector network analyser VSA vector signal analyser W-CDMA wideband code division multiple access viii List of Symbols a1 incident power wave at port-1 dBm a2 incident power wave at port-2 dBm b1 reflected power wave from port-1 dBm b2 reflected power wave from port-2 dBm β propagation coefficient C capacitance F Cgs intrinsic gate-source capacitance F Cds intrinsic drain-source capacitance F Cgd intrinsic gate-drain capacitance F C/I3 3rd-order carrier-to-intermodulation ratio dBc ∆f carrier spacing Hz ∆IMD IMD asymmetry dB εr dielectric constant e00 directivity e11 port-1 match e10 coupler tracking e01e10 reflection tracking e22 port-2 match fc centre frequency Hz fenv maximum baseband frequency Hz fSR series resonant frequency Hz Γ reflection coefficient ΓL load reflection coefficient G conductance S Gm transconductance S Gds channel conductance S nd Gm2, k2gm 2-order derivative of drain-source current S/V rd Gm3, k3gm 3-order derivative of drain-source current S/V² th hn time-domain n -order Volterra kernel th Hn frequency-domain n -order transfer function st H1 1-order linear transfer function Ids intrinsic incremental drain current A nd i2NL 2-order nonlinear current source A rd i3NL 3-order nonlinear current source A IDS,DC self-biased DC drain current A Imax channel saturation current A In excitation vector (voltage-controlled current source) IP3 3rd-order intercept point dBm k2g, k3g conductance nonlinearity coefficients k2c, k3c capacitance nonlinearity coefficients A transmission line length m ix LS capacitor’s parasitic inductance H M number of phase states Pin input power W Pout output power W P1dB 1 dB compression point dBm Q quality factor Qgs gate-source charge C Qgd gate-drain charge C Qg gate depletion charge C R resistance Ω t time sec TF, TFXYZ, transimpedance transfer function TFXYZW vg gate nodal voltage V vd drain nodal voltage V vs source nodal voltage V vgs incremental gate-source voltage V vds incremental drain-source voltage V vgd incremental gate-drain voltage V VBR gate-drain breakdown voltage V Vin input signal amplitude V VGS0 extrinsic gate-source bias voltage V VDS0 extrinsic drain-source bias voltage V VGS extrinsic gate-source voltage V VDS extrinsic drain-source voltage V Vk knee voltage V Vpi pinch-off voltage V Vt threshold voltage V vx(t) input signal amplitude vpeak(∆f ) peak baseband drain bias voltage V ω angular frequency Hz x(t) input excitation XL inductive reactance Ω XC capacitive reactance Ω y(t) output system response yNL(t) nonlinear output response yML(t) memoryless output response yQM(t) quasi-memoryless output response z(t) linear output response Z0 characteristic impedance Ω ZL load impedance Ω x Abstract Growing demand for higher data rates and ever increasing users on the 3G network is forcing rapid system enhancements to meet the stringent linearity specifications. The implications of microwave power transistor semiconductor technology and design strategies, implemented in basestation power amplifiers (PAs), have become the core focus of research. This thesis offers relevant practical application of computer-aided design (CAD) based modelling and measurement techniques to tackle linearity enhancement issues
Recommended publications
  • RF Measurement Concepts
    Published by CERN in the Proceedings of the CAS-CERN Accelerator School: Advanced Accelerator Physics, Trondheim, Norway, 19–29 August 2013, edited by W. Herr, CERN-2014-009 (CERN, Geneva, 2014) RF Measurement Concepts F. Caspers1 and P. Kowina2 1CERN, Geneva, Switzerland 2GSI, Darmstadt, Germany Abstract For the characterization of components, systems and signals in the radiofre- quency (RF) and microwave ranges, several dedicated instruments are in use. In this article the fundamentals of the RF signal techniques are discussed. The key element in these front ends is the Schottky diode which can be used either as a RF mixer or as a single sampler. The spectrum analyser has become an absolutely indispensable tool for RF signal analysis. Here the front end is the RF mixer as the RF section of modern spectrum analyses has a rather complex architecture. The reasons for this complexity and certain working principles as well as limitations are discussed. In addition, an overview of the develop- ment of scalar and vector signal analysers is given. For the determination of the noise temperature of a one-port and the noise figure of a two-port, basic concepts and relations are shown as well as a brief discussion of commonly used noise-measurement techniques. In a further part of this article the oper- ating principles of network analysers are shown. A distinction can be made between scalar and vector network analysers and their methods of measuring the transmission or reflection coefficients are explained. As digital signal pro- cessing has become cheap and easily available over the last 30 years, these instruments have become extremely versatile and powerful.
    [Show full text]
  • Vacuum Tubes Vs. Transistors
    Vacuum Tubes Vs. Transistors Is There An Audible Difference? Russell O. Hamm Journal of The Audio Engineering Society Presented September 14, 1972, at the 43rd Convention of the Audio Engineering Society, New York Abstract Engineers and musicians have long debated the question of tube sound versus transistor sound. Previous attempts to measure this difference have always assumed linear operation of the test amplifier. This conventional method of frequency response, distortion and noise measurement has shown that no significant difference exists. This paper, however, points out that amplifiers are often severely overloaded by signal transients (THD 30%). Under this condition there is a major difference in the harmonic distortion components of the amplified signal, with tubes, transistors, and operational amplifiers separating into distinct groups. Introduction As recording engineers we became directly involved with the tube sound versus transistor sound controversy as it related to pop recording. The difference became markedly noticeable as more solid-state consoles made their appearance. Of course there are so many sound problems related to studio acoustics that electronic problems are generally considered the least of one's worries. After acoustically rebuilding several studios, however, we began to question just how much of a role acoustics played. During one session in a studio notorious for bad sound we plugged the microphones into Ampex portable mixers instead of the regular console. The change in sound quality was nothing short of incredible. All the acoustic changes we had made in that studio never had brought about the vast improvement in the sound that a single change in electronics had.
    [Show full text]
  • Vacuum Tube & Distortion Emulation
    AdAddendum A19 Vacuum Tube & Distortion Emulation Part 2 Will Pirkle May 14, 2019 Copyright (c) 2019 Addendum A19 Designing Audio Effects Plugins in C++ Copyright © 2019 Will Pirkle Addendum Preface This addendum accompanies Will Pirkle’s Designing Audio Effects Plugins in C++, 2nd Edition. It specifically addresses material that was removed from Chapter 19 on nonlinear processing. Due to space limitations, the vacuum tube chapter had to be cut short and the projects slimmed down to simple wave shaping and filtering. I almost removed the entire chapter; however there has been demand for this kind of information. The reason I removed the material has to do with a special situation that happens with vacuum tubes in high-gain modern guitar amplifiers. In these designs, the engineers purposefully overdrive the inputs to the tube devices in order to create the modern distortion that is currently popular. In contrast, non-guitar tube-amp circuits are usually designed to stay within the proper operating conditions so that their inputs are not purposefully overdriven. When you overdrive the input to most amplifying devices like transistors or op-amps, once you’ve exceeded the operating limits, no more amplification will occur. The device simply won’t amplify the signal outside of its input range, and the signal is hard-clipped at that point. For a vacuum tube, this is true for the negative part of an over driven input signal. But when the positive portion of the input goes outside the limit, everything changes and the tube’s behavior becomes very dynamic. Cascading multiple overdriven stages together with differing amounts of gain between stages produces a very complex harmonic effect where the harmonic component amplitudes are directly linked to the signal amplitude.
    [Show full text]
  • University of Huddersfield Repository
    University of Huddersfield Repository Moore, Austin An Investigation into Non-Linear Sonic Signatures with a Focus on Dynamic Range Compression and the 1176 Fet Compressor Original Citation Moore, Austin (2017) An Investigation into Non-Linear Sonic Signatures with a Focus on Dynamic Range Compression and the 1176 Fet Compressor. Doctoral thesis, University of Huddersfield. This version is available at http://eprints.hud.ac.uk/id/eprint/34118/ The University Repository is a digital collection of the research output of the University, available on Open Access. Copyright and Moral Rights for the items on this site are retained by the individual author and/or other copyright owners. Users may access full items free of charge; copies of full text items generally can be reproduced, displayed or performed and given to third parties in any format or medium for personal research or study, educational or not-for-profit purposes without prior permission or charge, provided: • The authors, title and full bibliographic details is credited in any copy; • A hyperlink and/or URL is included for the original metadata page; and • The content is not changed in any way. For more information, including our policy and submission procedure, please contact the Repository Team at: [email protected]. http://eprints.hud.ac.uk/ AN INVESTIGATION INTO NON-LINEAR SONIC SIGNATURES WITH A FOCUS ON DYNAMIC RANGE COMPRESSION AND THE 1176 FET COMPRESSOR AUSTIN MOORE A thesis submitted to the University of Huddersfield in partial fulfilment of the requirements for the degree of Doctor of Philosophy The University of Huddersfield October 2017 ! Copyright statement 1.! The author of this thesis (including any appendices and/or schedules to this thesis) owns any copyright in it (the “Copyright”) and s/he has given The University of Huddersfield the right to use such copyright for any administrative, promotional, educational and/or teaching purposes.
    [Show full text]
  • ANSI/CTA Standard
    AANNSSII//CCTTAA SSttaannddaarrdd Standard Method of Measurement for In-Home Loudspeakers ANSI/CTA-2034-A (Formerly ANSI/CEA-2034-A) February 2015 NOTICE Consumer Technology Association (CTA)™ Standards, Bulletins and other technical publications are designed to serve the public interest through eliminating misunderstandings between manufacturers and purchasers, facilitating interchangeability and improvement of products, and assisting the purchaser in selecting and obtaining with minimum delay the proper product for his particular need. Existence of such Standards, Bulletins and other technical publications shall not in any respect preclude any member or nonmember of the Consumer Technology Association from manufacturing or selling products not conforming to such Standards, Bulletins or other technical publications, nor shall the existence of such Standards, Bulletins and other technical publications preclude their voluntary use by those other than Consumer Technology Association members, whether the standard is to be used either domestically or internationally. Standards, Bulletins and other technical publications are adopted by the Consumer Technology Association in accordance with the American National Standards Institute (ANSI) patent policy. By such action, the Consumer Technology Association does not assume any liability to any patent owner, nor does it assume any obligation whatever to parties adopting the Standard, Bulletin or other technical publication. This document does not purport to address all safety problems associated with its use or all applicable regulatory requirements. It is the responsibility of the user of this document to establish appropriate safety and health practices and to determine the applicability of regulatory limitations before its use. This document is copyrighted by the Consumer Technology Association and may not be reproduced, in whole or part, without written permission.
    [Show full text]
  • Achelous Mems Speakers Ut-P 2016 | Datasheet
    Released May 2019 ACHELOUS MEMS SPEAKERS UT-P 2016 | DATASHEET Achelous MEMS speaker is ideal for in-ear audio solutions such as wired earphones or true wireless systems (TWS). Thanks to its small size and lightweight, Achelous offers maximum flexibility for outstanding design approaches. As a speaker with a wide bandwidth it enables high-res audio applications. Achelous produces vivid, clear and rich sound, immersing the listener into their personal audio environment. FEATURES • Full bandwidth achieved by a single MEMS speaker • Enables modern, lightweight and ergonomic designs for wired earphones and TWS • Seamless integration into acoustics devices • Longer battery life due to the speaker low power consumption • Competitive sound pressure level • No magnetic field • Low heat generation APPLICATIONS • In-ear audio systems Released April 2019 TABLE OF CONTENT Components 3 Specifications 4 Test conditions 6 Acoustic performance in coupler (IEC 60318-4) 7 Acoustic performance using the Carme test box in coupler 8 Mechanical dimensions 9 Connectivity 10 Tracking 10 Handling and assembly recommendations 11 Important notice and disclaimer 12 Annex: THD assessment 13 REVISION HISTORY Released May 2019 COMPONENTS Figure 1: Achelous MEMS speaker components. 3 Released May 2019 SPECIFICATIONS MECHANICS Size [mm] 6.7 x 4.7 x 1.56 Total speaker weight [mg] 47 Total speaker cubic volume [mm3] 49 ACOUSTICS General fres @15 VP [kHz] 2.8 ±10% Q @ fres / 15 VP [-] 0.6 Effective membrane surface - SD [mm²] 12 Equivalent volume – VAS [mm³] 60 Front volume
    [Show full text]
  • Optimizing IP3 and ACPR Measurements
    Optimizing IP3 and ACPR Measurements Tips for Getting the Best Performance from Vector Signal Analyzers Optimizing IP3 and ACPR Measurements Tips for Getting the Best Performance from Vector Signal Analyzers Table of Contents 1. Overview ................................................................................................................................. 2 2. Theory of Intermodulation Distortion ................................................................................. 2 3. Optimizing IP3 Measurements ............................................................................................. 4 4. Theory of Adjacent Channel Power Ratio ........................................................................... 9 5. Optimizing ACPR Measurements ...................................................................................... 11 1 Visit www.ni.com/rf-academy Optimizing IP3 and ACPR Measurements Tips for Getting the Best Performance from Vector Signal Analyzers 1. Overview As wireless communication becomes widespread, the increased complexity of the devices and wireless protocols create an unrelenting demand for linear RF components and systems. These ubiquitous wireless devices require high performance test systems to characterize linearity. Linearity performance, particularly third order intercept point (IP3 or TOI), has become a defining characteristic as it affects power efficiency, channel density, signal coverage, and adjacent channel power ratio (ACPR). IP3 performance is a figure of merit used to describe the
    [Show full text]
  • Audio Measurement Handbook
    AUDIO MEASUREMENT HANDBOOK Bob Metzler Audio Precision, Inc. Copyright © 1993 Audio Precision. All rights reserved. Second edition for PDF, January, 2005. Audio Precision document number 0058.0003 r1 No part of this book may be reproduced or transmitted in any form or by any means, electronic or mechanical, including photocopying, recording, or by any information storage and retrieval system, without permission in writing from the publisher. Published by: AUDIO PRECISION 5750 SW Arctic Drive Beaverton, Oregon 97005 U.S.A. Telephone: (503) 627-0832 U.S. Toll-free telephone: (800) 231-7350 FAX: (503) 641-8906 Web site: audioprecision.com Printed in the United States of America V0127090352 ABOUT THIS BOOK The AUDIO MEASUREMENT HANDBOOK is intended as practical, hands-on assistance for workers in all phases of the audio field. Its treatment of topics does not involve mathematics beyond simple algebra. Although pub- lished by Audio Precision, the measurement techniques described generally are not specific to Audio Precision instruments, but apply to any audio testing equipment. The first section describes basic tools and techniques and includes guides to aid in the selection of appropriate audio test instruments. The second section discusses the common environments for audio testing. The third sec- tion applies these techniques to various commonly-used types of audio equip- ment and describes the typical ranges of performance to expect in that equip- ment. Section Four is a glossary of specific audio terminology and major speci- fications used in the audio measurement field. ABOUT THE COVER The classic audio test instruments on the cover are from the “museum” at Audio Precision.
    [Show full text]
  • Low Voltage Vacuum Tube Pre-Amplifier for Guitar from User Needs to a Commercialized Product
    Low Voltage Vacuum Tube Pre-Amplifier for Guitar From User Needs to a Commercialized Product Master of Science Thesis Eric Nolan Sporer Department of Product and Product Development Division of Product Development CHALMERS UNIVERSITY OF TECHNOLOGY Göteborg, Sweden, 2011 Low Voltage Vacuum Tube Pre-Amplifier for Guitar From User Needs to a Commercialized Product Eric Nolan Sporer Department of Product and Production Development CHALMERS UNIVERSITY OF TECHNOLOGY Göteborg, Sweden 2011 Low Voltage Vacuum Tube Pre-Amplifier for Guitar From User Needs to a Commercialized Product Eric Nolan Sporer © Eric Nolan Sporer, 2011. Department of Product and Production Development Chalmers University of Technology SE-412 96 Göteborg Sweden Telephone +46 (0)31-772 1000 Cover: Prototype of a distortion sound effect for guitar implementing a low voltage vacuum tube pre-amplifier Chalmers University of Technology Göteborg, Sweden 2011 Low Voltage Vacuum Tube Pre-Amplifier for Guitar From User Needs to a Commercialized Product Eric Nolan Sporer Department of Product and Production Development Chalmers University of Technology SUMMARY The vacuum tube was the first electrical signal amplification device. The solid state transistor, upon its invention, replaced the vacuum tube in most applications. Vacuum tubes, however, are still commonly found in guitar amplifiers due to their aurally pleasing non-linear behavior. Vacuum tubes require high voltages to operate properly; low voltage operation leads to extreme non-linearity which is not aurally pleasing. The high voltages necessary for proper operation have limited the use of vacuum tubes in guitar distortion sound effects due to the high costs associated with high voltage operation. In what was identified as a price sensitive market, opportunities were present to introduce products, including distortion sound effects, which can implement vacuum tubes at prices which are competitive with solid state devices.
    [Show full text]
  • Op Amps for Everyone
    Op Amps For Everyone Ron Mancini, Editor in Chief Design Reference August 2002 Advanced Analog Products SLOD006B IMPORTANT NOTICE Texas Instruments Incorporated and its subsidiaries (TI) reserve the right to make corrections, modifications, enhancements, improvements, and other changes to its products and services at any time and to discontinue any product or service without notice. Customers should obtain the latest relevant information before placing orders and should verify that such information is current and complete. All products are sold subject to TI’s terms and conditions of sale supplied at the time of order acknowledgment. TI warrants performance of its hardware products to the specifications applicable at the time of sale in accordance with TI’s standard warranty. Testing and other quality control techniques are used to the extent TI deems necessary to support this warranty. Except where mandated by government requirements, testing of all parameters of each product is not necessarily performed. TI assumes no liability for applications assistance or customer product design. Customers are responsible for their products and applications using TI components. To minimize the risks associated with customer products and applications, customers should provide adequate design and operating safeguards. TI does not warrant or represent that any license, either express or implied, is granted under any TI patent right, copyright, mask work right, or other TI intellectual property right relating to any combination, machine, or process in which TI products or services are used. Information published by TI regarding third party products or services does not constitute a license from TI to use such products or services or a warranty or endorsement thereof.
    [Show full text]
  • Linearization As a Solution for Power Amplifier Imperfections: a Review Of
    electronics Review Linearization as a Solution for Power Amplifier Imperfections: A Review of Methods Andžej Borel 1,2,* , Vaidotas Barzdenas˙ 1,2 and Aleksandr Vasjanov 1,2 1 Department of Computer Science and Communications Technologies, Vilnius Gediminas Technical University, 03227 Vilnius, Lithuania; [email protected] (V.B.); [email protected] (A.V.) 2 Micro and Nanoelectronics Systems Design and Research Laboratory, Vilnius Gediminas Technical University, 10223 Vilnius, Lithuania * Correspondence: [email protected] Abstract: Development of 5G networks requires a substantial increase to both spectral and power efficiency of transmitters. It is known that these two parameters are subjected to a mutual trade-off. To increase the linearity without losing power efficiency, linearization techniques are applied to power amplifiers. This paper aims to compare most popular linearization techniques to date and evaluate their applicability to upcoming 5G networks. The history of each respective linearization technique is followed by the main principle of operation, revealing advantages and disadvantages supported by concluding the latest research results. Three main groups of linearization methods currently known are feedforward, feedback, and predistortion, each with its own tradeoffs. Although digital predistortion seems to be the go-to method currently, other techniques with less research attention are still non-obsolete. A generalized discussion and a direct comparison of techniques analyzed are presented at the end of this paper. The article offers a systematic view on PA linearization problems which should be useful to researchers of this field. It is concluded that there are still a lot of problems Citation: Borel, A.; Barzdenas,˙ V.; that need to be addressed in every linearization technique in order to achieve 5G specifications.
    [Show full text]
  • Transfer-Function Measurement with Sweeps DIRECTOR’S CUT INCLUDING PREVIOUSLY UNRELEASED MATERIAL and SOME CORRECTIONS
    Transfer-Function Measurement with Sweeps DIRECTOR’S CUT INCLUDING PREVIOUSLY UNRELEASED MATERIAL AND SOME CORRECTIONS THE ORIGINAL HAS BEEN PUBLISHED IN J.AES, 2001 JUNE, P.443-471 SWEN MÜLLER, AES member, Institut für Technische Akustik, RWTH, 52056 Aachen, Germany AND PAULO MASSARANI Acoustic Testing Laboratory, INMETRO, Xerém, Duque de Caxias (RJ), Brazil Compared to using pseudo-noise signals, transfer function measurements using sweeps as excitation signal show significantly higher immunity against distortion and time variance. Capturing binaural room impulse responses for high-quality auralization purposes requires a signal-to-noise ratio of >90 dB which is unattainable with MLS- measurements due to loudspeaker non-linearity but fairly easy to reach with sweeps due to the possibility of completely rejecting harmonic distortion. Before investigating the differences and practical problems of measurements with MLS and sweeps and arguing why sweeps are the preferable choice for the majority of measurement tasks, the existing methods of obtaining transfer functions are reviewed. The continual need to use pre-emphasized excitation signals in acoustical measurements will also be addressed. A new method to create sweeps with arbitrary spectral contents, but constant or prescribed frequency-dependent temporal envelope is presented. Finally, the possibility of simultaneously analysing transfer function and harmonics is investigated. 1 0 INTRODUCTION Measuring transfer functions and their associated impulse responses (IRs) is one of the most important daily tasks in all areas of acoustics. The technique is practically needed everywhere. A loudspeaker developer will check the frequency response of a new prototype many times before releasing it for production. As the on-axis response does not sufficiently characterize a loudspeaker, a full set of polar data requiring many measurements is needed.
    [Show full text]