DAC and Vector Modulator DC offset calibration
|
|
- Branden McLaughlin
- 5 years ago
- Views:
Transcription
1 DAC and Vector Modulator DC calibration Zheqiao Geng March 9, 9 Introduction This is the algorithm to calibrate the DC of the DAC of the LLRF controller. The goals are Calibrate the DAC/VM DC automatically Study the possibility to calibrate onle (with terrupt operation) Phenomena Fig1 DC at FLASH klystron 5 Problems: Problems to set zero gradient DC is added to the feed forward signals, make difficulties to defe the feed forward tables Cause error for applications that take the decay data (assumg there is no power at the end of the RF pulse) Error Model V = I + jq V = I + jq Fig Drivg cha of the cavities Copyright 1 by MSK. Publication of any part of this document should be agreed by the authors
2 Fig3 Error model of the drivg cha Calibration Unknown parameters: I, Q : The of the I/Q channels, which have the same scale with feed forward table K i + j*k q : The complex ga from the feed forward signal to pick up signal (both are expressed by the sampled values) g, φ: The ga imbalance and phase imbalance of the vector modulator (potato effect the first order approximation) Known parameters: I, Q : The put signal generated by feed forward table I, Q : The put signal measured from the pick up pot (see Fig) ω: The RF signal frequency, which will not appear the calibration, only for better understandg of the Fig3 Calibration strategy: Lear fittg The formula for fittg is worked as below: The base band equation [( I + I ) + j( Q + Q )]( K jk ) I + jq = + (1) I = Ki Q = K ( I + I ) Kq( Q + Q ) ( I + I ) + K ( Q + Q ) q i And because of the put signal at the pick up pot is ( RF band) V () t = I cos( ωt) + gq s( ωt + ϕ) = I cos( t) + gq s( ωt) cos( ϕ) + gq cos( ωt) s(ϕ ω ) So, with the demodulation, the base band put signal can be written as I Q = I + gq = gq cos s( ϕ) ( ϕ) Put equation () to (4), we get the formula between put and put i q () (3) (4) Copyright 1 by MSK. Publication of any part of this document should be agreed by the authors. - -
3 where I Q = ai = ci + bq + dq + k + l a = Ki + Kq c = Kqg cos e = ai, f = bq m = ci, n = dq k = e + f, l = m + n g s( ϕ), b = Kq + Kig s( ϕ) ( ϕ), d = K g cos( ϕ) i From equation (5), there are 6 unknown parameters: a, b, c, d, k and l. So, we need 3 put/put vectors for calculatg these parameters. But the normal way is to generate more put vectors, measure the correspondg put vectors, and use lear fittg for better estimation of the unknown parameters. After gettg a, b, c, d, k and l, the of I/Q channels can be calculated from the equation below k = ai l = ci + bq + dq Also, from a, b, c, d, the complex ga, phase and amplitude imbalance can be estimated as (5) (6) (7) 1 cb Ki = a c d 1 + d c Kq = Ki d c g cos( ϕ) = Kq b + Kq g s( ϕ) = Ki (8) Matlab Code function [ki,kq,ioff,qoff,pha_imbalance,amp_imbalance] = nfun_cal_dac(i,q,i,q) %=================================================== % function to calibrate the DC %=================================================== pno = length(i); A = zeros(*pno, 6); B = zeros(*pno, 1); for ii = 1:pno Copyright 1 by MSK. Publication of any part of this document should be agreed by the authors
4 A(*ii-1, 1) = I(ii); A(*ii-1, ) = Q(ii); A(*ii-1, 3) = ; A(*ii-1, 4) = ; A(*ii-1, 5) = 1; A(*ii-1, 6) = ; A(*ii, 1) = ; A(*ii, ) = ; A(*ii, 3) = I(ii); A(*ii, 4) = Q(ii); A(*ii, 5) = ; A(*ii, 6) = 1; B(*ii-1) = I(ii); B(*ii) = Q(ii); end; X = A\B; a = X(1); b = X(); c = X(3); d = X(4); k = X(5); l = X(6); A1 = [a b; c d]; B1 = [k;l]; X1 = A1\B1; Ioff = X1(1); Qoff = X1(); % calculate other parameters ki = (a - c*b/d) / (1 + (c/d)^); kq = ki * c/d; gcosf = c / kq; gsf = (b + kq) / ki; pha_imbalance = atan(gsf / gcosf) * 18 / pi; amp_imbalance = abs(complex(gcosf, gsf)); Copyright 1 by MSK. Publication of any part of this document should be agreed by the authors
5 Test Results Fig4 Workg status of ACC1 Table1 Calibration results of different pot number I Q K i K q g φ / deg Gradient / MV/m 3 pots e e pots e e pots e e pots e e pots e e IQ put from the feed forward table, set pot gradient = 1 MV/m IQ put from the klystron forward signal measurement, set pot gradient = 1 MV/m Fig5 3 pots put and put IQ put from the feed forward table, set pot gradient = 1 MV/m IQ put from the klystron forward signal measurement, set pot gradient = 1 MV/m Copyright 1 by MSK. Publication of any part of this document should be agreed by the authors
6 Fig6 8 pots put and put x 1 4 IQ put from the feed forward table, set pot gradient = 5 MV/m IQ put from the klystron forward signal measurement, set pot gradient = 5 MV/m x Fig7 16 pots put and put x 1 4 IQ put from the feed forward table, set pot gradient = 5 MV/m IQ put from the klystron forward signal measurement, set pot gradient = 5 MV/m x Fig8 3 pots put and put IQ put from the feed forward table, set pot gradient = 1 MV/m IQ put from the klystron forward signal measurement, set pot gradient = 1 MV/m Fig9 64 pots put and put Future plan DC can be calibrated durg normal operation by troducg small calibration pulse after the ma RF pulse, see the Fig1. Copyright 1 by MSK. Publication of any part of this document should be agreed by the authors
7 5 x 14 Calibration pulse after the normal RF pulse by feed forward table Feed forward signal for normal RF pulse Amplitude / arbitrary unit Calibration pulse Time / μs Fig1 Calibration pulse References [1]. Personal discussion with Stefan Simrock Copyright 1 by MSK. Publication of any part of this document should be agreed by the authors
Cavity Field Control - Feedback Performance and Stability Analysis. LLRF Lecture Part3.2 S. Simrock, Z. Geng DESY, Hamburg, Germany
Cavity Field Control - Feedback Performance and Stability Analysis LLRF Lecture Part3.2 S. Simrock, Z. Geng DESY, Hamburg, Germany Motivation Understand how the perturbations and noises influence the feedback
More informationCavity Field Control - RF Field Controller. LLRF Lecture Part3.3 S. Simrock, Z. Geng DESY, Hamburg, Germany
Cavity Field Control - RF Field Controller LLRF Lecture Part3.3 S. Simrock, Z. Geng DESY, Hamburg, Germany Content Introduction to the controller Control scheme selection In-phase and Quadrature (I/Q)
More informationLow-Level RF. S. Simrock, DESY. MAC mtg, May 05 Stefan Simrock DESY
Low-Level RF S. Simrock, DESY Outline Scope of LLRF System Work Breakdown for XFEL LLRF Design for the VUV-FEL Cost, Personpower and Schedule RF Systems for XFEL RF Gun Injector 3rd harmonic cavity Main
More informationFLASH rf gun. beam generated within the (1.3 GHz) RF gun by a laser. filling time: typical 55 μs. flat top time: up to 800 μs
The gun RF control at FLASH (and PITZ) Elmar Vogel in collaboration with Waldemar Koprek and Piotr Pucyk th FLASH Seminar at December 19 2006 FLASH rf gun beam generated within the (1.3 GHz) RF gun by
More informationSoftware Design Specification for LLRF Applications at FLASH Version 1.0 Prepared by Zheqiao Geng MSK, DESY Nov. 16, 2009
Software Design Specification for LLRF Applications at FLASH Version 1.0 Prepared by Zheqiao Geng MSK, DESY Nov. 16, 2009 Copyright 2009 by Zheqiao Geng. Any change of this document should be agreed by
More informationSoftware Requirements Specification for LLRF Applications at FLASH Version 1.0 Prepared by Zheqiao Geng MSK, DESY Nov. 06, 2009
Software Specification for LLRF Applications at FLASH Version 1.0 Prepared by Zheqiao Geng MSK, DESY Nov. 06, 2009 Copyright 2009 by Zheqiao Geng. Any change of this document should be agreed by the development
More informationMIMO-LTI Feedback Controller Design -Status report-
MIMO-LTI Feedback Controller Design -Status report- Christian Schmidt Deutsches Elektronen Synchrotron Technische Universitaet Hamburg Harburg FLASH Seminar 4/1/28 Outline Current RF Feedback System MIMO
More informationSuperconducting cavity driving with FPGA controller
TESLA-FEL 26-7 Superconducting cavity driving with FPGA controller Tomasz Czarski, Waldemar Koprek, Krzysztof T. Poźniak, Ryszard S. Romaniuk, Warsaw University of Technology Stefan Simrock, Alexander
More informationBorut Baricevic. Libera LLRF. 17 September 2009
Borut Baricevic Libera LLRF borut.baricevic@i-tech.si 17 September 2009 Outline Libera LLRF introduction Libera LLRF system topology Signal processing structure GUI and signal acquisition RF system diagnostics
More informationNormal-conducting high-gradient rf systems
Normal-conducting high-gradient rf systems Introduction Motivation for high gradient Order of 100 GeV/km Operational and state-of-the-art SwissFEL C-band linac: Just under 30 MV/m CLIC prototypes: Over
More informationCOMPLEX ENVELOPE CONTROL OF PULSED ACCELERATING FIELD
Tomasz Czarski COMPLEX ENVELOPE CONTROL OF PULSED ACCELERATING FIELD IN SUPERCONDUCTING CAVITY RESONATORS L = 9 λ/2 ~ 1037 particle (z,τ) E 0 (z) 0 z Institute of Electronic Systems Publishing House of
More informationState of the Art in RF Control
State of the Art in RF Control S. Simrock, DESY LINAC 2004, Lübeck Stefan Simrock DESY Outline RF System Architecture Requirements for RF Control RF Control Design Considerations Design Efforts Worldwide
More informationImprovements of the LLRF system at FLASH. Mariusz Grecki, Waldemar Koprek and LLRF team
Improvements of the LLRF system at FLASH Mariusz Grecki, Waldemar Koprek and LLRF team Agenda GUN linearization Adaptive feed-forward at ACC1 Beam load compensation at ACC1 Klystron nonlinearity compensation
More informationCircuit Analysis-II. Circuit Analysis-II Lecture # 2 Wednesday 28 th Mar, 18
Circuit Analysis-II Angular Measurement Angular Measurement of a Sine Wave ü As we already know that a sinusoidal voltage can be produced by an ac generator. ü As the windings on the rotor of the ac generator
More informationCalibrating the Cavity Voltage. Presentation of an idea
Calibrating the Cavity Voltage. Presentation of an idea Stefan Wilke, DESY MHF-e 21st ESLS rf meeting Kraków, 15th/16th nov 2017 Accelerators at DESY. linear and circular Page 2 Accelerators at DESY. linear
More informationDigital Signal Processing in RF Applications
Digital Signal Processing in RF Applications Part II Thomas Schilcher Outline 1. signal conditioning / down conversion 2. detection of amp./phase by digital I/Q sampling I/Q sampling non I/Q sampling digital
More informationSNS LLRF Design Experience and its Possible Adoption for the ILC
SNS LLRF Design Experience and its Possible Adoption for the ILC Brian Chase SNS - Mark Champion Fermilab International Linear Collider Workshop 11/28/2005 1 Why Consider the SNS System for ILC R&D at
More informationAn Iterative Learning Algorithm for Control of an Accelerator Based Free Electron Laser
Proceedings of the 47th IEEE Conference on Decision and Control Cancun, Mexico, Dec. 9-, 8 WeB5.5 An Iterative Learning Algorithm for Control of an Accelerator Based Free Electron Laser S. Kichhoff, C.
More informationDigital LLRF Test on the Renascence Cryomodule
Digital LLRF Test on the Renascence Cryomodule Trent Allison, Rama Bachimanchi, Curt Hovater, John Musson and Tomasz Plawski Introduction The Renascence cryomodule was the first opportunity for testing
More informationTutorial on RF (Receiver Fundamentals) Frank Ludwig DESY
Frank Ludwig DESY Outline Introduction to Noise and Systems Front-Ends Components Receiver Structures Distortions and Reduction Techniques Motivation Field regulation and noise sources : Beam energy jitter
More informationReview on Progress in RF Control Systems. Cornell University. Matthias Liepe. M. Liepe, Cornell U. SRF 2005, July 14
Review on Progress in RF Control Systems Matthias Liepe Cornell University 1 Why this Talk? As we all know, superconducting cavities have many nice features one of which is very high field stability. Why?
More informationThe low level radio frequency control system for DC-SRF. photo-injector at Peking University *
The low level radio frequency control system for DC-SRF photo-injector at Peking University * WANG Fang( 王芳 ) 1) FENG Li-Wen( 冯立文 ) LIN Lin( 林林 ) HAO Jian-Kui( 郝建奎 ) Quan Sheng-Wen( 全胜文 ) ZHANG Bao-Cheng(
More informationRF Systems I. Erk Jensen, CERN BE-RF
RF Systems I Erk Jensen, CERN BE-RF Introduction to Accelerator Physics, Prague, Czech Republic, 31 Aug 12 Sept 2014 Definitions & basic concepts db t-domain vs. ω-domain phasors 8th Sept, 2014 CAS Prague
More informationFor my parents
Ì Ò Ð ÍÒ Ú Ö ØÝ Ó ÄÓ Þ Ì ÙÐØÝ Ó Ð ØÖ Ð Ð ØÖÓÒ ÓÑÔÙØ Ö Ò ÓÒØÖÓÐ Ò Ò Ö Ò Ô ÖØÑ ÒØ Ó Å ÖÓ Ð ØÖÓÒ Ò ÓÑÔÙØ Ö Ë Ò È Û È ÛÐ ÅË Ð Ö Ø Ò Ð ØÖ Ð ØÖ Ò Ø ÑÔÐ ØÙ Ò Ô Ð Ö Ø ÓÒ ÓÒ Ô ÖØ Ð Ñ Ò Ù Ð ØÖ Ð ØÖ Ò Ø ØÖ Ò ÒØ Ø
More informationDigital Low Level RF for SESAME
Technical Sector Synchrotron-light for Experimental Science And Applications in the Middle East Subject : RF More specified area: Digital Low Level RF Date: 6/23/2010 Total Number of Pages: 11 Document
More informationField Stability Issue for Normal Conducting Cavity under Beam Loading
Field Stability Issue for Normal Conducting Cavity under Beam Loading Rihua Zeng, 3- - Introduction There is cavity field blip at the beginning of beam loading (~several ten micro-seconds) under PI control
More informationExtending Vector Signal Analysis to 26.5 GHz with 20 MHz Information Bandwidth Product Note
H Extending Vector Signal Analysis to 26.5 GHz with 20 MHz Information Bandwidth Product Note 89400-13 The HP 89400 series vector signal analyzers provide unmatched signal analysis capabilities from traditional
More informationSmall Signal Amplifiers - BJT. Definitions Small Signal Amplifiers Dimensioning of capacitors
Small Signal mplifiers BJT Defitions Small Signal mplifiers Dimensiong of capacitors 1 Defitions (1) Small signal condition When the put signal (v and, i ) is small so that output signal (v out and, i
More informationTo produce more powerful and high-efficiency particle accelerator, efforts have
Measuring Unloaded Quality Factor of Superconducting RF Cryomodule Jian Cong Zeng Department of Physics and Astronomy, State University of New York at Geneseo, Geneseo, NY 14454 Elvin Harms, Jr. Accelerator
More informationEXPERIMENTAL RESULT OF LORENTZ DETUNING IN STF PHASE-1 AT KEK-STF
EXPERIMENTAL RESULT OF LORENTZ DETUNING IN STF PHASE-1 AT KEK-STF Y. Yamamoto #, H. Hayano, E. Kako, T. Matsumoto, S. Michizono, T. Miura, S. Noguchi, M. Satoh, T. Shishidio, K. Watanabe, KEK, Tsukuba,
More informationAbstract. Keywords: Super conducting cavity control, signal conversion, FPGA, DSP, optics fibers, FPGA with optical I/O, free electron laser, FEL
EU contract number RII3-CT-2003-506395 CARE Conf-04-046-SRF SRF FPGA and optical network based LLRF distributed control system for TESLA-XFEL Linear Accelerator Krzysztof T. Pozniak, Ryszard S. Romaniuk,
More informationLab Assignment 2 Phase-sensitive Rectifier (Lock-in Amplifier) Objective. Equipment Required. A. Theoretical Introduction
Lab Assignment Phase-sensitive Rectifier (Lock- Amplifier By: Prof. Dr. rer. nat. habil. Albrecht Rost niversity of Applied Sciences Merseburg Department 1: Computer Science and Applied Natural Sciences
More informationTests and Measurements II: Distortion
Tests and Measurements II: Distortion.1 Introduction A lot of changes have been made to the methodologies used for testg for distortion modern RF-contag SoC devices. Many excellent resources are available
More informationDesign and performance of LLRF system for CSNS/RCS *
Design and performance of LLRF system for CSNS/RCS * LI Xiao 1) SUN Hong LONG Wei ZHAO Fa-Cheng ZHANG Chun-Lin Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, China Abstract:
More informationAutomatic phase calibration for RF cavities using beam-loading signals. Jonathan Edelen LLRF 2017 Workshop (Barcelona) 18 Oct 2017
Automatic phase calibration for RF cavities using beam-loading signals Jonathan Edelen LLRF 2017 Workshop (Barcelona) 18 Oct 2017 Introduction How do we meet 10-4 energy stability for PIP-II? 2 11/9/2017
More informationMicrophonics. T. Powers
Microphonics T. Powers What is microphonics? Microphonics is the time domain variation in cavity frequency driven by external vibrational sources. A 1.5 GHz structure 0.5 m long will change in frequency
More informationINTRA-TRAIN LONGITUDINAL FEEDBACK FOR BEAM STABILIZATION AT FLASH
INTRA-TRAIN LONGITUDINAL FEEDBACK FOR BEAM STABILIZATION AT FLASH W. Koprek*, C. Behrens, M. K. Bock, M. Felber, P. Gessler, K. Hacker, H. Schlarb, C. Schmidt, B. Steffen, S. Wesch, DESY, Hamburg, Germany
More information1 GSW Noise and IP3 in Receivers
Gettg Started with Communications Engeerg GSW Noise and 3 Receivers GSW Noise and 3 Receivers In many cases, the designers of dividual receiver components (mostly amplifiers, mixers and filters) don t
More information14 What You Should Know About Decibels
14 What You Should Know About Decibels Every year dozens of students who should know much better lose a lot of exam marks because they haven t grasped the concept of the decibel. This is a great pity:
More informationStatus of superconducting module development suitable for cw operation: ELBE cryostats
Status of superconducting module development suitable for cw operation: ELBE cryostats, A. Büchner, H. Büttig, F. Gabriel, P. Michel, K. Möller, U. Lehnert, Ch. Schneider, J. Stephan, A. Winter Forschungszentrum
More informationA Simplified Extension of X-parameters to Describe Memory Effects for Wideband Modulated Signals
Jan Verspecht bvba Mechelstraat 17 B-1745 Opwijk Belgium email: contact@janverspecht.com web: http://www.janverspecht.com A Simplified Extension of X-parameters to Describe Memory Effects for Wideband
More informationRLC Circuits. Centre College. Physics 230 Lab 8
ircuits entre ollege Phsics 230 ab 8 1 Preliminaries Objective To stud the electrical characteristics of an alternating current circuit containing a resistor, inductor, and capacitor. Equipment Oscilloscope,
More informationTheory and Practice of Cavity Test Systems. Tom Powers
Theory and Practice of Cavity Test Systems Tom Powers SRF Workshop 2005 Tutorial Session INTRODUCTION Over the past 17 years we have done about 2500 cold cavity tests on more than 500 different cavities
More informationFourier Transform. louder softer. louder. softer. amplitude. time. amplitude. time. frequency. frequency. P. J. Grandinetti
Fourier Transform * * amplitude louder softer amplitude louder softer frequency frequency Fourier Transform amplitude What is the mathematical relationship between two signal domains frequency Fourier
More informationBaseband simulation model of the vector rf voltage control system for the J-PARC RCS
Journal of Physics: Conference Series PAPER OPEN ACCESS Baseband simulation model of the vector rf voltage control system for the J-PARC RCS To cite this article: Fumihiko Tamura et al 2018 J. Phys.: Conf.
More informationFLASH. FLASH Training: RF Gun. FLASH: the first soft X-ray FEL operating two undulator beamlines simultaneously. Siegfried Schreiber, DESY
FLASH Training: RF Gun FLASH: the first soft X-ray FEL operating two undulator beamlines simultaneously Siegfried Schreiber, DESY FLASH Training DESY 17-Mar-2017 FLASH1 RF Gun History RF Guns operated
More informationDigital Signal Analysis
Digital Signal Analysis Objectives - Provide a digital modulation overview - Review common digital radio impairments Digital Modulation Overview Signal Characteristics to Modify Polar Display / IQ Relationship
More informationInternational Conference on Automation, Mechanical Control and Computational Engineering (AMCCE 2015)
International Conference on Automation, Mechanical Control and Computational Engineering (AMCCE 1) Design of Digital Phase-locking Amplifier Applied in Detection of Weak Photoelectric Signals Lei Wang,
More informationAll-in-one solution for RFID, baseband, and IF signals
R&S FMU36 Baseband Signal nalyzer ll-in-one solution for RFID, baseband, and IF signals The R&S FMU36 offers developers a variety of analysis capabilities as it includes an FFT spectrum analyzer and a
More information04th - 16th August, th International Nathiagali Summer College 1 CAVITY BASICS. C. Serpico
39th International Nathiagali Summer College 1 CAVITY BASICS C. Serpico 39th International Nathiagali Summer College 2 Outline Maxwell equations Guided propagation Rectangular waveguide Circular waveguide
More informationHIGH POWER COUPLER FOR THE TESLA TEST FACILITY
Abstract HIGH POWER COUPLER FOR THE TESLA TEST FACILITY W.-D. Moeller * for the TESLA Collaboration, Deutsches Elektronen-Synchrotron DESY, D-22603 Hamburg, Germany The TeV Energy Superconducting Linear
More informationINSTALLATION AND FIRST COMMISSIONING OF THE LLRF SYSTEM
INSTALLATION AND FIRST COMMISSIONING OF THE LLRF SYSTEM FOR THE EUROPEAN XFEL Julien Branlard, for the LLRF team TALK OVERVIEW 2 Introduction Brief reminder about the XFEL LLRF system Commissioning goals
More informationLLRF Plans for SMTF. Ruben Carcagno (Fermilab) Nigel Lockyer (University of Pennsylvania) Thanks to DESY, PISA, KEK, Fermilab, SLAC Colleagues
LLRF Plans for SMTF Ruben Carcagno (Fermilab) Nigel Lockyer (University of Pennsylvania) Thanks to DESY, PISA, KEK, Fermilab, SLAC Colleagues Outline Near-term (< 1.5 years) SMTF LLRF plan Long-term (>
More informationDigital Self Excited Loop Implementation and Experience. Trent Allison Curt Hovater John Musson Tomasz Plawski
Digital Self Excited Loop Implementation and Experience Trent Allison Curt Hovater John Musson Tomasz Plawski Overview Why Self Excited Loop? Algorithm Building Blocks Hardware and Sampling Digital Signal
More informationDouble-Resonance Magnetometry in Arbitrarily Oriented Fields. Stuart Ingleby University of Strathclyde
Ingleby, Stuart and Riis, Erling and Arnold, Aidan and Griffin, Paul and O'Dwyer, Carolyn and Chalmers, Iain (2017) Double-resonance magnetometry in arbitrarily oriented fields. In: Workshop on Optically
More informationALICE SRF SYSTEM COMMISSIONING EXPERIENCE A. Wheelhouse ASTeC, STFC Daresbury Laboratory
ALICE SRF SYSTEM COMMISSIONING EXPERIENCE A. Wheelhouse ASTeC, STFC Daresbury Laboratory ERL 09 8 th 12 th June 2009 ALICE Accelerators and Lasers In Combined Experiments Brief Description ALICE Superconducting
More informationHigh acceleration gradient. Critical applications: Linear colliders e.g. ILC X-ray FELs e.g. DESY XFEL
High acceleration gradient Critical applications: Linear colliders e.g. ILC X-ray FELs e.g. DESY XFEL Critical points The physical limitation of a SC resonator is given by the requirement that the RF magnetic
More informationDigital Signal Processing Techniques
Digital Signal Processing Techniques Dmitry Teytelman Dimtel, Inc., San Jose, CA, 95124, USA June 17, 2009 Outline 1 Introduction 2 Signal synthesis Arbitrary Waveform Generation CORDIC Direct Digital
More informationBeam Diagnostics, Low Level RF and Feedback for Room Temperature FELs. Josef Frisch Pohang, March 14, 2011
Beam Diagnostics, Low Level RF and Feedback for Room Temperature FELs Josef Frisch Pohang, March 14, 2011 Room Temperature / Superconducting Very different pulse structures RT: single bunch or short bursts
More informationInitial Beam Phasing of the SRF Cavities in LCLS-II
Introduction Initial Beam Phasing of the SRF Cavities in LCLS-II P. Emma Nov. 28, 2016 One of the more challenging aspects of commissioning the LCLS-II accelerator is in the initial phasing of the SRF
More informationDESCRIPTION OF THE OPERATION AND CALIBRATION OF THE MILLIMETER I/Q PHASE BRIDGE-INTERFEROMETER
DESCRIPTION OF THE OPERATION AND CALIBRATION OF THE MILLIMETER I/Q PHASE BRIDGE-INTERFEROMETER Overview of Interferometer Operation The block diagram of the I/Q Phase Bridge-Interferometer is shown below
More informationPhase demodulation using the Hilbert transform in the frequency domain
Phase demodulation using the Hilbert transform in the frequency domain Author: Gareth Forbes Created: 3/11/9 Revision: The general idea A phase modulated signal is a type of signal which contains information
More informationElectromagnetic Spectrum
Electromagnetic Spectrum The electromagnetic radiation covers a vast spectrum of frequencies and wavelengths. This includes the very energetic gamma-rays radiation with a wavelength range from 0.005 1.4
More informationTriarchy VSG6G1C USB Vector RF Signal Generator Operating Manual
Triarchy VSG6G1C USB Vector RF Signal Generator Operating Manual CW signal NB RF noise generator Analog modulation GMSK modulation Frequency sweeping Hopping with data Mod Page 1 of 27 8PSK GSM signal
More informationChapter 2 Shunt Active Power Filter
Chapter 2 Shunt Active Power Filter In the recent years of development the requirement of harmonic and reactive power has developed, causing power quality problems. Many power electronic converters are
More informationLLRF Operation and Performance of the European XFEL. An overview
LLRF Operation and Performance of the European XFEL. An overview Mathieu Omet LLRF, Barcelona, 16.10.2017 Contents > Introduction > LLRF commissioning > Energy Reach > LLRF performance > Summary / Outlook
More informationDigital Logic, Algorithms, and Functions for the CEBAF Upgrade LLRF System Hai Dong, Curt Hovater, John Musson, and Tomasz Plawski
Digital Logic, Algorithms, and Functions for the CEBAF Upgrade LLRF System Hai Dong, Curt Hovater, John Musson, and Tomasz Plawski Introduction: The CEBAF upgrade Low Level Radio Frequency (LLRF) control
More informationMartin Salter Centre for Electromagnetic and Time Metrology, National Physical Laboratory
Measuring signals close to the noise floor Martin Salter Centre for Electromagnetic and Time Metrology, National Physical Laboratory 1 Introduction The presence of noise in a microwave measurement receiver
More informationVibration studies of a superconducting accelerating
Vibration studies of a superconducting accelerating module at room temperature and at 4.5 K Ramila Amirikas, Alessandro Bertolini, Wilhelm Bialowons Vibration studies on a Type III cryomodule at room temperature
More informationTrig Graphs. What is a Trig graph? This is the graph of a trigonometrical function e.g.
Trig Graphs What is a Trig graph? This is the graph of a trigonometrical function e.g. sin, cos or tan How do we draw one? We make a table of value using the calculator. Tr to complete the one below (work
More informationLC Technology Hans Weise / DESY
LC Technology Hans Weise / DESY All you need is... Luminosity! L σ 2 N e x σ y σ y σ x L n b f rep Re-writing reflects the LC choices... L P E b c. m. N e σ σ x y... beam power... bunch population... Ac-to-beam
More informationINVESTIGATING THE USRP: I/Q IMBALANCE
INVESTIGATING THE USRP: I/Q IMBALANCE Peter Händel and Per Zetterberg Signal Processing Lab ACCESS Linnaeus Center Royal Institute of Technology Stockholm, Sweden RFMTC09, October 6-7, 2009, Gävle, Sweden.
More informationLab 8 6.S02 Spring 2013 MRI Projection Imaging
1. Spin Echos 1.1 Find f0, TX amplitudes, and shim settings In order to acquire spin echos, we first need to find the appropriate scanner settings using the FID GUI. This was all done last week, but these
More informationPUBLICATION. A Novel Approach for Automatic Control of Piezoelectric Elements Used for Lorentz Force Detuning Compensation
EuCARD-CON-21-4 European Coordination for Accelerator Research and Development PUBLICATION A Novel Approach for Automatic Control of Piezoelectric Elements Used for Lorentz Force Detuning Compensation
More informationSynchronization Overview
Synchronization Overview S. Simrock, DESY ERL Workshop 2005 Stefan Simrock DESY What is Synchronization Outline Synchronization Requirements for RF, Laser and Beam Timing stability RF amplitude and phase
More informationDSP Predistortion for a High-Efficiency Outphasing Transmitter
Event: PA IEEE 24 Date: 56 September 24 RC: IRR TBD DSP Predistortion for a High-Efficiency Outphasg Transmitter Authors: Advanced Technology Center John Reyland David Cripe Pr. Electrical Engeer Pr. Electrical
More informationIncreasing the Photon Energy for Photonuclear Experiments in MAX-lab by Phase Modulating the SLED Pulse
Increasing the Photon Energy for Photonuclear Experiments in MAX-lab by Phase Modulating the SLED Pulse Olsson, David; Lilja, Per; Malmgren, Lars 2016 Link to publication Citation for published version
More informationLesson 12: LRC Circuit, Tuning and ode45
Lesson 12: LRC Circuit, Tuning and ode45 12.1 Applied Problem. A series LRC circuit can be viewed as a primitive tuning circuit in a simple radio. The objective is to adjust L or C so that the in the circuit
More informationThe Formula for Sinusoidal Signals
The Formula for I The general formula for a sinusoidal signal is x(t) =A cos(2pft + f). I A, f, and f are parameters that characterize the sinusoidal sinal. I A - Amplitude: determines the height of the
More informationAcceleration of High-Intensity Protons in the J-PARC Synchrotrons. KEK/J-PARC M. Yoshii
Acceleration of High-Intensity Protons in the J-PARC Synchrotrons KEK/J-PARC M. Yoshii Introduction 1. J-PARC consists of 400 MeV Linac, 3 GeV Rapid Cycling Synchrotron (RCS) and 50 GeV Main synchrotron
More informationEXPLORING THE MAXIMUM SUPERHEATING MAGNETIC FIELDS OF NIOBIUM
EXPLORING THE MAXIMUM SUPERHEATING MAGNETIC FIELDS OF NIOBIUM N. Valles, Z. Conway, M. Liepe, Cornell University, CLASSE, Ithaca, NY 14853, USA Abstract The RF superheating magnetic field of superconducting
More informationLLRF Controls and Feedback: Free-Electron Lasers and Energy Recovery Linacs
Proceedings of the CAS CERN Accelerator School: Free Electron Lasers and Energy Recovery Linacs, Hamburg, Germany, 31 May 10 June 2016, edited by R. Bailey, CERN Yellow Reports: School Proceedings, Vol.
More informationMicrowave Technology
GUC (Dr. Hany Hammad) 9/5/06 Microwave Technology (COMM 903) Contents Introduction: Course contents. Assessment. eferences. Microwave Sources. Transistor Model Extraction. Signal flow graphs. COMM (903)
More informationHIGH POWER PULSED TESTS OF A BETA=0.5 5-CELL 704 MHZ SUPERCONDUCTING CAVITY
HIGH POWER PULSED TESTS OF A BETA=0.5 5-CELL 704 MHZ SUPERCONDUCTING CAVITY G. Devanz, D. Braud, M. Desmons, Y. Gasser, E. Jacques, O. Piquet, J. Plouin, J.- P. Poupeau, D. Roudier, P. Sahuquet, CEA-Saclay,
More informationLinac Coherent Light Source (LCLS) Low Level RF Status LCLS FAC. October 30, 2007
Linac Coherent Light Source (LCLS) Low Level RF Status LCLS Emma LCLS RF Gun, L0, and L1 Emma Dual Feed L0A L0B L0A 57MV 19MV/m L0B 72MV 24MV/m Off Axis Injector Vault Injector Transverse Accelerator 55cm
More informationA Simplified Extension of X-parameters to Describe Memory Effects for Wideband Modulated Signals
A Simplified Extension of X-parameters to Describe Memory Effects for Wideband Modulated Signals Jan Verspecht*, Jason Horn** and David E. Root** * Jan Verspecht b.v.b.a., Opwijk, Vlaams-Brabant, B-745,
More informationTransceiver Architectures (III)
Image-Reject Receivers Transceiver Architectures (III) Since the image and the signal lie on the two sides of the LO frequency, it is possible to architect the RX so that it can distinguish between the
More informationJørgen S. Nielsen Center for Storage Ring Facilities (ISA) Aarhus University Denmark. ESLS-RF 22 (8/ ), ASTRID2 RF system 1
Jørgen S. Nielsen Center for Storage Ring Facilities (ISA) Aarhus University Denmark ESLS-RF 22 (8/11 2018), ASTRID2 RF system 1 ASTRID2 is the new synchrotron light source in Aarhus, Denmark, since 2013
More informationarxiv: v1 [physics.data-an] 9 Jan 2008
Manuscript prepared for Ann. Geophys. with version of the L A TEX class copernicus.cls. Date: 27 October 18 arxiv:080343v1 [physics.data-an] 9 Jan 08 Transmission code optimization method for incoherent
More informationSlide Title. Bulleted Text
Slide Title 1 Slide Outline Title Brief view of the C-AD Complex Review of the RHIC LLRF Upgrade Platform Generic Implementation of a Feedback Loop RHIC Bunch by Bunch Longitudinal Damper Cavity Controller
More informationWaveguide Arc Restrike Test Results Abstract Background
Waveguide Arc Restrike Test Results Tom Powers, Doug Curry, Kirk Davis, Larry King, and Mike Tiefenback Thomas Jefferson National Accelerator Facility (Test dates July 6, 2004 through September 2, 2004)
More informationDigital Phase Control Techniques for Accelerator Cavities.
Digital Phase Control Techniques for Accelerator Cavities. Amos Dexter, Imran Tahir, Graeme Burt and Richard Carter Lancaster University Engineering Department Abstract RF cavities used for the acceleration
More informationAdvance on High Power Couplers for SC Accelerators
Advance on High Power Couplers for SC Accelerators Eiji Kako (KEK, Japan) IAS conference at Hong Kong for High Energy Physics, 2017, January 23th Eiji KAKO (KEK, Japan) IAS at Hong Kong, 2017 Jan. 23 1
More informationDesign of a Transceiver for 3G DECT Physical Layer. - Rohit Budhiraja
Design of a Transceiver for 3G DECT Physical Layer - Rohit Budhiraja The Big Picture 2G DECT Binary GFSK 1.152Mbps 3G DECT M-ary DPSK 3.456 Mbps DECT - Digital Enhanced Cordless Telecommunications Overview
More informationProgress Report on SIMULINK Modelling of RF Cavity Control for SPL Extension to LINAC4
Progress Report on SIMULINK Modelling of RF Cavity Control for SPL Extension to LINAC4 Theory and Analysis behind Simulation Results of SPL Model Using I/Q Components in SIMULINK to Date, Including Lorentz
More informationProgress Report on SIMULINK Modelling of RF Cavity Control for SPL Extension to LINAC4
EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH European Laboratory for Particle Physics slhc Project slhc Project Report 0054 Progress Report on SIMULINK Modelling of RF Cavity Control for SPL Extension to
More informationA Signal Space Theory of Interferences Cancellation Systems
A Signal Space Theory of Interferences Cancellation Systems Osamu Ichiyoshi Human Network for Better 21 Century E-mail: osamu-ichiyoshi@muf.biglobe.ne.jp Abstract Interferences among signals from different
More informationPaul Scherrer Institute Pierre-André Duperrex. On-line calibration schemes for RF-based beam diagnostics
Paul Scherrer Institute Pierre-André Duperrex On-line calibration schemes for RF-based beam diagnostics HB2012 Beijing, 17-20 Sept. 2012 Motivation Current monitor Some difficulties related to RF signal
More informationMeasurement Setup for Bunched Beam Echoes in the HERA Proton Storage Ring
Measurement Setup for Bunched Beam Echoes in the HERA Proton Storage Ring 1 Measurement Setup for Bunched Beam Echoes in the HERA Proton Storage Ring Elmar Vogel, Wilhelm Kriens and Uwe Hurdelbrink Deutsches
More informationIn a typical biological sample the concentration of the solute is 1 mm or less. In many situations,
Water suppression n a typical biological sample the concentration of the solute is 1 mm or less. n many situations, the signals of interest are those of amide protons that exchange with the solvent water.
More information