MAX II RF system 100 MHz technology Lars Malmgren 10th ESLS RF Meeting Dortmund September 27-28, 2006

Size: px
Start display at page:

Download "MAX II RF system 100 MHz technology Lars Malmgren 10th ESLS RF Meeting Dortmund September 27-28, 2006"

Transcription

1 MAX II RF system 1 MHz technology Lars Malmgren 1th ESLS RF Meeting Dortmund September 27-28, 26

2 Facts and figures MAX-II Frequency [MHz] Harmonic number No of cavity cells No of transmitters Cell radius [m] Tot length of cavities [m] Tot R shunt ( V*V/P) [MΩ] Q-value Tot Voltage [kv] Cu losses [kw] Beam 25mA [kw] Available power [kw] Net power [kw] Bucket height [%] Synchrotron frequency [khz] Rms bunch length [cm] (53) 21 (29) 35 (5) 9 93(135)

3 Simple circuit model of the RFsystem with beam Z c =cavity impedance Z Z c L coup L C R s I beam n λ/2 L coup << L β = R Z S L coup L Z R = βs L coup L N 2 N=transformer ratio

4 RF-system with beamloading Z = 2 I + U c R β Z sinφ + s i Q DC s 1 ξ 2 I U DC c R s cosφ s Φ s is the phase angle between the synchronous electron and the zero crossing of the cavity voltage. A. Matched condition of resistive part: ReZ=Z 2 IDC RS β = 1+ sinφs UC 2 I U R 2 R P β = 1+ sinφ = 1+ P = 1+ DC C S S beam 2 S 2 beam UC UC PC B. Matched condition of reactive part: ImZ= 2 f 2 I DC Rs Q ξ = Q = cosφs f U c C A. Defines the coupling factor of the cavity B. Defines the necessary detuning of the cavity

5 Cavity A. The main cavities are of the capacity-loaded type. B. The tuning is made by squeezing the cavity side.

6 1 MHz cavity 1 MHz Capacity-loaded Cavity for MAX-II and -III, F = MHz C:\LANL\EXAMPLES\RADIOFREQUENCY\PILLBOXCAVITIES\1MHZ.AF :3:5 1 MHz cavity profile with fundamental mode E-field lines 1 MHz Capacity-loaded Cavity for MAX-II and -III, F = MHz Q-value 19 Tot. R shunt 3.2 MΩ C:\LANL\EXAMPLES\RADIOFREQUENCY\PILLBOXCAVITIES\1MHZ.AF :16:42 E-field lines of the high order mode at 456 MHz 5 The high order modes are damped by antennas in the endplate. This endplate is convenient to use since the fundamental mode is not affected.

7 Landau cavity The Landau cavities are of simple pill-box type. Tuning is done both by plunger and temperature.

8 RF amplifier and feeder line The generator system consists of three 3 kw FM transmitters (Itelco T254T) feeding one cavity each The power stages are tetrode amplifiers Class C operation for high efficiency An integer λ/2 long coaxial 3 1/8 transmission line is feeding the cavity input coupler. The reflected wave will add in phase with the wave at the generator

9 RF path φ φ Power amplifier Phase control loop 1 MHz master oscillator Main cavity Power control loop Single stub tuner Frequency tuning loop The power control makes the cavity to see a matched condition at the generator. A phase control system is used to control the phase difference between the cavities.

10 Stub matching network A stub matching network is installed to keep an optimal match of transmitter and cavity for every beam current.

11 An alternative to a circulator λ/4 +n λ S 3 db hybrid Dummy load Dummy load Switchless combiner Tetrode amplifiers

12 BPM system Band pass filter 3 MHz Low pass filter ADC Multiplexer Demultiplexer ADC From buttons Analog Signal Processing ADC ADC The BPM receivers are working at the third harmonic. This minimizes the risk of 1 MHz leakage from the transmitters. Resolution << 1µm

13 CONCLUSION The 1 MHz 9 kw RF system has been in operation since September 24. The system is now running at 24 ma with two wigglers at 15 and 2A. Beam lifetime I*t=6mAh with Landau cavity in operation. BPM system resolution <<1 µm. The transmitter tubes must have high anode loss capability when working without circulator. This is an disadvantage but a solution is presented.

Detailed Design Report

Detailed Design Report Detailed Design Report Chapter 2 MAX IV 3 GeV Storage Ring 2.6. The Radio Frequency System MAX IV Facility CHAPTER 2.6. THE RADIO FREQUENCY SYSTEM 1(15) 2.6. The Radio Frequency System 2.6. The Radio Frequency

More information

Tutorial on Design of RF system for Indus Accelerator. Maherdra Lad Head, Radio Frequency Systems Division RRCAT, Indore

Tutorial on Design of RF system for Indus Accelerator. Maherdra Lad Head, Radio Frequency Systems Division RRCAT, Indore Tutorial on Design of RF system for Indus Accelerator Maherdra Lad Head, Radio Frequency Systems Division RRCAT, Indore Basic principle of RF Acceleration RF Power Amplifier The RF source supplies power

More information

Jørgen S. Nielsen Institute for Storage Ring Facilities, Aarhus, University of Aarhus Denmark

Jørgen S. Nielsen Institute for Storage Ring Facilities, Aarhus, University of Aarhus Denmark Jørgen S. Nielsen Institute for Storage Ring Facilities, Aarhus, University of Aarhus Denmark What is ISA? ISA operates and develops the storage ring ASTRID and related facilities ISA staff assist internal

More information

Project of RF System for 2.2 GeV Electron Storage Ring Zelenograd SR Source.

Project of RF System for 2.2 GeV Electron Storage Ring Zelenograd SR Source. Project of RF System for 2.2 GeV Electron Storage Ring Zelenograd SR Source. I.K. Sedlyarov V.S. Arbuzov, E.I Gorniker, A.A. Kondakov, S.A. Krutikhin, G.Ya. Kurkin, I.V.Kuptsov, V.N. Osipov, V.M. Petrov,

More information

Calibrating the Cavity Voltage. Presentation of an idea

Calibrating 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 information

New apparatus for precise synchronous phase shift measurements in storage rings 1

New apparatus for precise synchronous phase shift measurements in storage rings 1 New apparatus for precise synchronous phase shift measurements in storage rings 1 Boris Podobedov and Robert Siemann Stanford Linear Accelerator Center, Stanford University, Stanford, CA 94309 Measuring

More information

Jørgen 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/ ), 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 information

Main Injector Cavity Simulation and Optimization for Project X

Main Injector Cavity Simulation and Optimization for Project X Main Injector Cavity Simulation and Optimization for Project X Liling Xiao Advanced Computations Group Beam Physics Department Accelerator Research Division Status Meeting, April 7, 2011 Outline Background

More information

1.5 GHz Cavity design for the Clic Damping Ring and as Active Third Harmonic cavity for ALBA.

1.5 GHz Cavity design for the Clic Damping Ring and as Active Third Harmonic cavity for ALBA. 1 1.5 GHz Cavity design for the Clic Damping Ring and as Active Third Harmonic cavity for ALBA. Beatriz Bravo Overview 2 1.Introduction 2.Active operation 3.Electromagnetic design 4.Mechanical design Introduction

More information

Superstructures; First Cold Test and Future Applications

Superstructures; First Cold Test and Future Applications Superstructures; First Cold Test and Future Applications DESY: C. Albrecht, V. Ayvazyan, R. Bandelmann, T. Büttner, P. Castro, S. Choroba, J. Eschke, B. Faatz, A. Gössel, K. Honkavaara, B. Horst, J. Iversen,

More information

Predictions of LER-HER limits

Predictions of LER-HER limits Predictions of LER-HER limits PEP-II High Current Performance T. Mastorides, C. Rivetta, J.D. Fox, D. Van Winkle Accelerator Technology Research Div., SLAC 2e 34 Meeting, May 2, 27 Contents In this presentation

More information

Multi-bunch feedback systems

Multi-bunch feedback systems Multi-bunch feedback systems M. Lonza Elettra Synchrotron Light Laboratory, Sincrotrone Trieste S.C.p.A., Trieste, Italy Abstract Coupled-bunch instabilities excited by the interaction of the particle

More information

Introduction to Synchrotron Radio Frequency System

Introduction to Synchrotron Radio Frequency System 3 rd ILSF Advanced School on Synchrotron Radiation and Its Applications September 14-16, 2013 Introduction to Synchrotron Radio Frequency System Khorshid Sarhadi Head of ILSF RF Group 15 Sep. 2013 1 Outline

More information

Lawrence Berkeley Laboratory UNIVERSITY OF CALIFORNIA

Lawrence Berkeley Laboratory UNIVERSITY OF CALIFORNIA d e Lawrence Berkeley Laboratory UNIVERSITY OF CALIFORNIA Accelerator & Fusion Research Division I # RECEIVED Presented at the International Workshop on Collective Effects and Impedance for B-Factories,

More information

2008 JINST 3 S The RF systems and beam feedback. Chapter Introduction

2008 JINST 3 S The RF systems and beam feedback. Chapter Introduction Chapter 4 The RF systems and beam feedback 4.1 Introduction The injected beam will be captured, accelerated and stored using a 400 MHz superconducting cavity system, and the longitudinal injection errors

More information

Longitudinal bunch shape Overview of processing electronics for Beam Position Monitor (BPM) Measurements:

Longitudinal bunch shape Overview of processing electronics for Beam Position Monitor (BPM) Measurements: Pick-Ups for bunched Beams The image current at the beam pipe is monitored on a high frequency basis i.e. the ac-part given by the bunched beam. Beam Position Monitor BPM equals Pick-Up PU Most frequent

More information

Design and performance of LLRF system for CSNS/RCS *

Design 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 information

Bunch-by-Bunch Broadband Feedback for the ESRF

Bunch-by-Bunch Broadband Feedback for the ESRF Bunch-by-Bunch Broadband Feedback for the ESRF ESLS RF meeting / Aarhus 21-09-2005 J. Jacob, E. Plouviez, J.-M. Koch, G. Naylor, V. Serrière Goal: Active damping of longitudinal and transverse multibunch

More information

FAST RF KICKER DESIGN

FAST RF KICKER DESIGN FAST RF KICKER DESIGN David Alesini LNF-INFN, Frascati, Rome, Italy ICFA Mini-Workshop on Deflecting/Crabbing Cavity Applications in Accelerators, Shanghai, April 23-25, 2008 FAST STRIPLINE INJECTION KICKERS

More information

10th ESLS RF Meeting September ALBA RF System. F. Perez. on behalf of the ALBA RF Group. ALBA RF System 1/21

10th ESLS RF Meeting September ALBA RF System. F. Perez. on behalf of the ALBA RF Group. ALBA RF System 1/21 ALBA RF System F. Perez on behalf of the ALBA RF Group ALBA RF System 1/21 Synchrotron Light Source in Cerdanyola (Barcelona, Spain) 3 GeV accelerator 30 beamlines (7 on day one) 50-50 Spanish Government

More information

780-8 Series Constant Impedance FM Combiners

780-8 Series Constant Impedance FM Combiners Features Cylindrical construction provides better mechanical and electrical stability than square or rectangular cavities Factory tuned to customer s specified channel, yet can be easily field converted

More information

MEASURES TO REDUCE THE IMPEDANCE OF PARASITIC RESONANT MODES IN THE DAΦNE VACUUM CHAMBER

MEASURES TO REDUCE THE IMPEDANCE OF PARASITIC RESONANT MODES IN THE DAΦNE VACUUM CHAMBER Frascati Physics Series Vol. X (1998), pp. 371-378 14 th Advanced ICFA Beam Dynamics Workshop, Frascati, Oct. 20-25, 1997 MEASURES TO REDUCE THE IMPEDANCE OF PARASITIC RESONANT MODES IN THE DAΦNE VACUUM

More information

Multi-bunch Feedback Systems

Multi-bunch Feedback Systems Multi-bunch Feedback Systems M. Lonza, presented by H. Schmickler Elettra Synchrotron Light Laboratory, Sincrotrone Trieste S.C.p.A., Trieste, Italy Abstract Coupled-bunch instabilities excited by the

More information

Position of the LHC luminous region

Position of the LHC luminous region Position of the LHC luminous region SL/HRF reported by Philippe Baudrenghien Philippe Baudrenghien SL-HRF 1 RF low-level during physics (tentative...) Good lifetime -> One phase loop per beam... - Goal

More information

1997 Particle Accelerator Conference, Vancouver, B.C., Canada, May 12-16, 1997 BNL

1997 Particle Accelerator Conference, Vancouver, B.C., Canada, May 12-16, 1997 BNL t J 1997 Particle Accelerator Conference, Vancouver, B.C., Canada, May 12-16, 1997 BNL-6 4 3 5 5 Modifying CERN SPS Cavities and Amplifiers for Use in RHIC R. Connolly, J. Aspenleiter, S. Kwiatkowski Brookhaven

More information

O. Napoly LC02, SLAC, Feb. 5, Higher Order Modes Measurements

O. Napoly LC02, SLAC, Feb. 5, Higher Order Modes Measurements O. Napoly LC02, SLAC, Feb. 5, 2002 Higher Order Modes Measurements with Beam at the TTF Linac TTF Measurements A collective effort including most of Saclay, Orsay and DESY TTF physicists : S. Fartoukh,

More information

Low-Level RF. S. Simrock, DESY. MAC mtg, May 05 Stefan Simrock DESY

Low-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 information

J. Jacob: Status of the ESRF RF upgrade

J. Jacob: Status of the ESRF RF upgrade 17th ESLS RF Meeting 2013 HZB BESSY 18th 19th September Status of the ESRF RF upgrade J. Jacob J.-M. Mercier V. Serrière M. Langlois G. Gautier [CINEL] 1 RF upgrade phase 1 until 2015 - reminder Replacement

More information

EC 1402 Microwave Engineering

EC 1402 Microwave Engineering SHRI ANGALAMMAN COLLEGE OF ENGINEERING & TECHNOLOGY (An ISO 9001:2008 Certified Institution) SIRUGANOOR,TRICHY-621105. DEPARTMENT OF ELECTRONICS AND COMMUNICATION ENGINEERING EC 1402 Microwave Engineering

More information

5/1.0 kw AM Transmitter

5/1.0 kw AM Transmitter 5/1.0 kw AM Transmitter Collins' 820E /F -1 series of broadcast transmitters is one of the most extensively transistorized series of transmitters available in the 5 -kw to 10 -kw power range. The series

More information

Resonator System for the BEST 70MeV Cyclotron

Resonator System for the BEST 70MeV Cyclotron Resonator System for the BEST 70MeV Cyclotron 20 nd International Conference on Cyclotrons and their Applications Vancouver, Canada, September 16-20, 2013 Vasile Sabaiduc, Dipl. Eng. Accelerator Technology

More information

R.K.YADAV. 2. Explain with suitable sketch the operation of two-cavity Klystron amplifier. explain the concept of velocity and current modulations.

R.K.YADAV. 2. Explain with suitable sketch the operation of two-cavity Klystron amplifier. explain the concept of velocity and current modulations. Question Bank DEPARTMENT OF ELECTRONICS AND COMMUNICATION SUBJECT- MICROWAVE ENGINEERING(EEC-603) Unit-III 1. What are the high frequency limitations of conventional tubes? Explain clearly. 2. Explain

More information

PAUL SCHERRER INSTITUT

PAUL SCHERRER INSTITUT PAUL SCHERRER INSTITUT Contents: 1. Introduction 2. The initial normal conducting system 3. Possible further upgrading 3.1 Superconducting RF cavities 3.2 The hybrid powered nc and idle sc RF system 3.2.1

More information

LHC TRANSVERSE FEEDBACK SYSTEM: FIRST RESULTS OF COMMISSIONING. V.M. Zhabitsky XXI Russian Particle Accelerator Conference

LHC TRANSVERSE FEEDBACK SYSTEM: FIRST RESULTS OF COMMISSIONING. V.M. Zhabitsky XXI Russian Particle Accelerator Conference LHC TRANSVERSE FEEDBACK SYSTEM: FIRST RESULTS OF COMMISSIONING V.M. Zhabitsky XXI Russian Particle Accelerator Conference 28.09-03.10.2008, Zvenigorod LHC Transverse Feedback System: First Results of Commissioning

More information

Third Harmonic Superconducting passive cavities in ELETTRA and SLS

Third Harmonic Superconducting passive cavities in ELETTRA and SLS RF superconductivity application to synchrotron radiation light sources Third Harmonic Superconducting passive cavities in ELETTRA and SLS 2 cryomodules (one per machine) with 2 Nb/Cu cavities at 1.5 GHz

More information

3. (a) Derive an expression for the Hull cut off condition for cylindrical magnetron oscillator. (b) Write short notes on 8 cavity magnetron [8+8]

3. (a) Derive an expression for the Hull cut off condition for cylindrical magnetron oscillator. (b) Write short notes on 8 cavity magnetron [8+8] Code No: RR320404 Set No. 1 1. (a) Compare Drift space bunching and Reflector bunching with the help of Applegate diagrams. (b) A reflex Klystron operates at the peak of n=1 or 3 / 4 mode. The dc power

More information

The Amazing MFJ 269 Author Jack Tiley AD7FO

The Amazing MFJ 269 Author Jack Tiley AD7FO The Amazing MFJ 269 Author Jack Tiley AD7FO ARRL Certified Emcomm and license class Instructor, Volunteer Examiner, EWA Technical Coordinator and President of the Inland Empire VHF Club What Can be Measured?

More information

Circumference 187 m (bending radius = 8.66 m)

Circumference 187 m (bending radius = 8.66 m) 4. Specifications of the Accelerators Table 1. General parameters of the PF storage ring. Energy 2.5 GeV (max 3.0 GeV) Initial stored current multi-bunch 450 ma (max 500 ma at 2.5GeV) single bunch 70 ma

More information

Beam Instability Investigations at DELTA

Beam Instability Investigations at DELTA 10 th ESLS-RF Meeting, September 27-28, Dortmund Beam Instability Investigations at Thomas Weis for the group Dortmund University Synchrotron Radiation Center Content: Status of the Facility Instability

More information

MICROWAVE MICROWAVE TRAINING BENCH COMPONENT SPECIFICATIONS:

MICROWAVE MICROWAVE TRAINING BENCH COMPONENT SPECIFICATIONS: Microwave section consists of Basic Microwave Training Bench, Advance Microwave Training Bench and Microwave Communication Training System. Microwave Training System is used to study all the concepts of

More information

CHAPTER 6 BOOSTER RF SYSTEMS

CHAPTER 6 BOOSTER RF SYSTEMS CHAPTER 6 BOOSTER RF SYSTEMS 6.1 NEW PSB RF CAVITIES H = 1 (0.6 1.8 MHz) The addition of cavities accelerating on RF harmonic h = 1 and supplemented with a h = 2 system, contributed to the reduction of

More information

Status of superconducting module development suitable for cw operation: ELBE cryostats

Status 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 information

Transmitter Tetrode TH 347

Transmitter Tetrode TH 347 Coaxial metal-ceramic tetrode, forced-air-cooled, for frequencies up to 1000 MHz. The tube is especially suitable for TV transmitters and TV translators, band IV/V. Dimensions in mm Approx. weight 2,3

More information

Status of the MAX IV RF systems. PPT-mall 2

Status of the MAX IV RF systems. PPT-mall 2 Status of the MAX IV RF systems PPT-mall 2 Lars Malmgren Med linje On Behalf of the MAX IV RF Group Åke Andersson, Joel Andersson, Richard Grandford, Sven-Olof Heed, Per Lilja, Dionis Kumbaro, Lars Malmgren,

More information

ERLP Status. Mike Dykes

ERLP Status. Mike Dykes ERLP Status Mike Dykes Content ASTeC RF & Diagnostics Group Work of the Group 4GLS ERLP Photo-injector Accelerating Modules Summary High Power RF Engineering Andy Moss SRS Support; DIAMOND; ERLP; MICE;

More information

COMMUNICATION SYSTEMS NCERT

COMMUNICATION SYSTEMS NCERT Exemplar Problems Physics Chapter Fifteen COMMUNCATON SYSTEMS MCQ 151 Three waves A, B and C of frequencies 1600 khz, 5 MHz and 60 MHz, respectively are to be transmitted from one place to another Which

More information

TitleThe RF Power Amplifier System for a Author(s) Fujisawa, Hiroshi Citation Bulletin of the Institute for Chemi University (1991), 69(1): 11-14 Issue Date 1991-03-30 URL http://hdl.handle.net/2433/77367

More information

Paul 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 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 information

ERI FM Band Pass Filters

ERI FM Band Pass Filters ERI 780-3 FM Band Pass Filters Features Cylindrical construction provides better mechanical and electrical stability than square or rectangular cavities Factory tuned to customer s specified channel, yet

More information

Fundamental mode rejection in SOLEIL dipole HOM couplers

Fundamental mode rejection in SOLEIL dipole HOM couplers Fundamental mode rejection in SOLEIL dipole HOM couplers G. Devanz, DSM/DAPNIA/SACM, CEA/Saclay, 91191 Gif-sur-Yvette 14th June 2004 1 Introduction The SOLEIL superconducting accelerating cavity is a heavily

More information

UNIT Write short notes on travelling wave antenna? Ans: Travelling Wave Antenna

UNIT Write short notes on travelling wave antenna? Ans:   Travelling Wave Antenna UNIT 4 1. Write short notes on travelling wave antenna? Travelling Wave Antenna Travelling wave or non-resonant or aperiodic antennas are those antennas in which there is no reflected wave i.e., standing

More information

RF Design of Normal Conducting Deflecting Cavity

RF Design of Normal Conducting Deflecting Cavity RF Design of Normal Conducting Deflecting Cavity Valery Dolgashev (SLAC), Geoff Waldschmidt, Ali Nassiri (Argonne National Laboratory, Advanced Photon Source) 48th ICFA Advanced Beam Dynamics Workshop

More information

Automatic 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 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 information

TV combiners. Combiners with mask filters for digital operation TYPE DESCRIPTION

TV combiners. Combiners with mask filters for digital operation TYPE DESCRIPTION TV combiners TYPE DESCRIPTION 1 2-3 4-5 1-Number of inputs: 2PX - two inputs 3PX - three inputs 4PX - four inputs 5PX - five inputs 6PX - six inputs 7PX - seven inputs 8PX - eight inputs 9PX - nine inputs

More information

Bunch-by-bunch studies at DELTA

Bunch-by-bunch studies at DELTA Bunch-by-bunch studies at DELTA November 17 19, 29 Author: Dmitry Teytelman Revision: 1.2 March 3, 21 Copyright Dimtel, Inc., 21. All rights reserved. Dimtel, Inc. 259 Camden Avenue, Suite 136 San Jose,

More information

Welcome to AntennaSelect Volume 1 August 2013

Welcome to AntennaSelect Volume 1 August 2013 Welcome to AntennaSelect Volume 1 August 2013 This is the first issue of our new periodic newsletter, AntennaSelect. AntennaSelect will feature informative articles about antennas and antenna technology,

More information

EE 3324 Electromagnetics Laboratory

EE 3324 Electromagnetics Laboratory EE 3324 Electromagnetics Laboratory Experiment #10 Microstrip Circuits and Measurements 1. Objective The objective of Experiment #8 is to investigate the application of microstrip technology. A precision

More information

Transmitter Tetrode. Approx. weight 16 kg. 360 Siemens Aktiengesellschaft. ➀ Tube support ➁ Air inlet ➂ Do not use as terminal.

Transmitter Tetrode. Approx. weight 16 kg. 360 Siemens Aktiengesellschaft. ➀ Tube support ➁ Air inlet ➂ Do not use as terminal. Transmitter Tetrode RS 2795 Ordering code Q53-X2795 Coaxial metal-ceramic tetrode, forced-air-cooled, for frequencies up to 110 MHz, particularly suitable for single-sideband communications transmitters

More information

JC-5 4KW PEP, 1KW RMS AUTO ANTENNA COUPLER

JC-5 4KW PEP, 1KW RMS AUTO ANTENNA COUPLER JC-5 4KW PEP, 1KW RMS AUTO ANTENNA COUPLER 1) DIRECTLY CONTROLLED BY ICOM, ALINCO & KENWOOD. 2) INDEPENDENT CAPACITOR INPUT AND OUTPUT BLOCKS! 3) 3 mm COIL WIRE & INTERNAL FAN FOR THE BIG COILS! 4) DIPPED

More information

SPECTRACOM MODEL 8165 DISCIPLINED OSCILLATOR ANTENNA INSTALLATION TABLE OF CONTENTS

SPECTRACOM MODEL 8165 DISCIPLINED OSCILLATOR ANTENNA INSTALLATION TABLE OF CONTENTS SPECTRACOM MODEL 8165 DISCIPLINED OSCILLATOR ANTENNA INSTALLATION TABLE OF CONTENTS Page 1.0 INTRODUCTION... 1 1.3 MODEL 8206A LOOP ANTENNA... 1 1.4 MODEL 8208 WHIP ANTENNA... 4 1.5 ANTENNA LOCATION...

More information

REVIEW OF HIGH POWER CW COUPLERS FOR SC CAVITIES. S. Belomestnykh

REVIEW OF HIGH POWER CW COUPLERS FOR SC CAVITIES. S. Belomestnykh REVIEW OF HIGH POWER CW COUPLERS FOR SC CAVITIES S. Belomestnykh HPC workshop JLAB, 30 October 2002 Introduction Many aspects of the high-power coupler design, fabrication, preparation, conditioning, integration

More information

High Power Antenna Design for Lower Hybrid Current Drive in MST

High Power Antenna Design for Lower Hybrid Current Drive in MST High Power Antenna Design for Lower Hybrid Current Drive in MST M.A. Thomas, J.A. Goetz, M.C. Kaufman, S.P. Oliva University of WisconsinMadison J.B.O. Caughman, P.M. Ryan Oak Ridge National Laboratory

More information

RF Upgrade at DELTA. P. Hartmann DELTA, TU Dortmund

RF Upgrade at DELTA. P. Hartmann DELTA, TU Dortmund RF Upgrade at DELTA P. Hartmann DELTA, TU Dortmund DELTA parameters: Personnel: Beam energy: 550 MeV 1.5 GeV Beam current: 130mA @ 1.5GeV Beam lifetime: 12h @ 130 ma Availability: 95 % Operational: 3000

More information

AC Dispersion Measurement. David Rubin Cornell Laboratory for Accelerator-Based Sciences and Education

AC Dispersion Measurement. David Rubin Cornell Laboratory for Accelerator-Based Sciences and Education AC Dispersion Measurement David Rubin Cornell Laboratory for Accelerator-Based Sciences and Education AC dispersion measurement Traditional dispersion measurement - Measure orbit - Change ring energy (δe/e

More information

STABILITY CONSIDERATIONS

STABILITY CONSIDERATIONS Abstract The simple theory describing the stability of an RF system with beam will be recalled together with its application to the LEP case. The so-called nd Robinson stability limit can be pushed by

More information

The BESSY Higher Order Mode Damped Cavity - Further Improvements -

The BESSY Higher Order Mode Damped Cavity - Further Improvements - The BESSY Higher Order Mode Damped Cavity - Further Improvements - Ernst Weihreter Reminder of Technical Problems Solutions Conclusions BESSY HOM Damped Cavity Project collaboration: (EC funded) - BESSY

More information

A Technical Report: Jampro s Dual Input Interleaved HD FM antenna:

A Technical Report: Jampro s Dual Input Interleaved HD FM antenna: A Technical Report: Jampro s Dual Input Interleaved HD FM antenna: This JMPC-2 + JMPC-2-HD is shown installed on a 24 triangle tower. Many other configurations are available to meet your HD Radio Needs.

More information

Project X Cavity RF and mechanical design. T. Khabiboulline, FNAL/TD/SRF

Project X Cavity RF and mechanical design. T. Khabiboulline, FNAL/TD/SRF Project X Cavity RF and mechanical design T. Khabiboulline, FNAL/TD/SRF TTC meeting on CW-SRF, 2013 Project X Cavity RF and mechanical design T 1 High ß Low ß 0.5 HWR SSR1 SSR2 0 1 10 100 1 10 3 1 10 4

More information

RF System Models and Longitudinal Beam Dynamics

RF System Models and Longitudinal Beam Dynamics RF System Models and Longitudinal Beam Dynamics T. Mastoridis 1, P. Baudrenghien 1, J. Molendijk 1, C. Rivetta 2, J.D. Fox 2 1 BE-RF Group, CERN 2 AARD-Feedback and Dynamics Group, SLAC T. Mastoridis LLRF

More information

Performance of the Prototype NLC RF Phase and Timing Distribution System *

Performance of the Prototype NLC RF Phase and Timing Distribution System * SLAC PUB 8458 June 2000 Performance of the Prototype NLC RF Phase and Timing Distribution System * Josef Frisch, David G. Brown, Eugene Cisneros Stanford Linear Accelerator Center, Stanford University,

More information

A WAVEGUIDE OVERLOADED CAVITY AS LONGITUDINAL KICKER FOR THE DAΦNE BUNCH-BY-BUNCH FEEDBACK SYSTEM

A WAVEGUIDE OVERLOADED CAVITY AS LONGITUDINAL KICKER FOR THE DAΦNE BUNCH-BY-BUNCH FEEDBACK SYSTEM International Workshop on Collective Effects and Impedance for B-Factories, Tsukuba, Japan, June 1995 A WAVEGUIDE OVERLOADED CAVITY AS LONGITUDINAL KICKER FOR THE DAΦNE BUNCH-BY-BUNCH FEEDBACK SYSTEM A.

More information

Cavity BPM With Dipole-Mode Selective Coupler

Cavity BPM With Dipole-Mode Selective Coupler Cavity BPM With Dipole-Mode Selective Coupler Zenghai Li Advanced Computations Department Stanford Linear Accelerator Center Presented at PAC23 Portland, Oregon. May 12-16, 23 Work supported by the U.S.

More information

Code No: R Set No. 1

Code No: R Set No. 1 Code No: R05220405 Set No. 1 II B.Tech II Semester Regular Examinations, Apr/May 2007 ANALOG COMMUNICATIONS ( Common to Electronics & Communication Engineering and Electronics & Telematics) Time: 3 hours

More information

The design of a radio frequency quadrupole LINAC for the RIB project at VECC Kolkata

The design of a radio frequency quadrupole LINAC for the RIB project at VECC Kolkata PRAMANA cfl Indian Academy of Sciences Vol. 59, No. 6 journal of December 2002 physics pp. 957 962 The design of a radio frequency quadrupole LINAC for the RIB project at VECC Kolkata V BANERJEE 1;Λ, ALOK

More information

Summary LOI Developments

Summary LOI Developments The 8th Collaboration Meeting on the 2nd Harmonic RF System July 4, 2003, ISIS Summary LOI Developments 1996 through 2003 1. Introduction why the Low Output Impedance? 2. History of the scheme (1) cathode

More information

NanoBPM tests in the ATF extraction line

NanoBPM tests in the ATF extraction line NLC - The Next Linear Collider Project NanoBPM tests in the ATF extraction line Calibrate movers (tilters) and BPM s Understand and test dynamic range and resolution June 2003 Marc Ross What are the uses

More information

A Technical Report: Jampro s Dual Input Shared Aperture HD FM antenna:

A Technical Report: Jampro s Dual Input Shared Aperture HD FM antenna: A Technical Report: Jampro s Dual Input Shared Aperture HD FM antenna: This JMPC-2 + JMPC-2-HD is shown installed on a 24 triangle tower. Many other configurations are available to meet your HD Radio Needs.

More information

Uppsala, June 17 th - 19 th, 2013

Uppsala, June 17 th - 19 th, 2013 TIARA Workshop on RF Power Generation for Accelerators Uppsala, June 17 th - 19 th, 2013 Massamba DIOP, R. LOPES, P. MARCHAND, F. RIBEIRO SSA operation at SOLEIL BOOSTER 35 kw STORAGE RING 180 kw SOLEIL

More information

Continental's 816R -5B, 35 kw Single Tube Broadcast Transmitter. Includes the 802A solid -state exciter

Continental's 816R -5B, 35 kw Single Tube Broadcast Transmitter. Includes the 802A solid -state exciter Continental's 816R -5B, 35 kw Single Tube Broadcast Transmitter Includes the 802A solid -state exciter LED status indicators Features SCR Power Control Automatic RF Power Output Control Automatic SWR Circuit

More information

Status of the 1.5 GeV Synchrotron Light Source DELTA and Related Accelerator Physics Activities

Status of the 1.5 GeV Synchrotron Light Source DELTA and Related Accelerator Physics Activities Status of the 1.5 GeV Synchrotron Light Source and Related Accelerator Physics Activities 2006 RuPAC, September 10-14, Novosibirsk Thomas Weis for the machine and accelerator physics group Dortmund University

More information

Application Note Receivers MLX71120/21 With LNA1-SAW-LNA2 configuration

Application Note Receivers MLX71120/21 With LNA1-SAW-LNA2 configuration Designing with MLX71120 and MLX71121 receivers using a SAW filter between LNA1 and LNA2 Scope Many receiver applications, especially those for automotive keyless entry systems require good sensitivity

More information

Understanding and Optimizing Electromagnetic Compatibility in Switchmode Power Supplies

Understanding and Optimizing Electromagnetic Compatibility in Switchmode Power Supplies Understanding and Optimizing Electromagnetic Compatibility in Switchmode Power Supplies 1 Definitions EMI = Electro Magnetic Interference EMC = Electro Magnetic Compatibility (No EMI) Three Components

More information

Beam 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 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 information

RF Systems I. Erk Jensen, CERN BE-RF

RF 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 information

Gyroklystron Research at CCR

Gyroklystron Research at CCR Gyroklystron Research at CCR RLI@calcreek.com Lawrence Ives, Michael Read, Jeff Neilson, Philipp Borchard and Max Mizuhara Calabazas Creek Research, Inc. 20937 Comer Drive, Saratoga, CA 95070-3753 W. Lawson

More information

General License Class Chapter 6 - Antennas. Bob KA9BHD Eric K9VIC

General License Class Chapter 6 - Antennas. Bob KA9BHD Eric K9VIC General License Class Chapter 6 - Antennas Bob KA9BHD Eric K9VIC Learning Objectives Teach you enough to get all the antenna questions right during the VE Session Learn a few things from you about antennas

More information

Multi-bunch Feedback Systems

Multi-bunch Feedback Systems Multi-bunch Feedback Systems Marco Lonza Sincrotrone Trieste - Elettra 1 Outline Coupled-bunch instabilities Basics of feedback systems Feedback system components Digital signal processing Integrated diagnostic

More information

Booster High-level RF Frequency Tracking Improvement Via the Bias-Curve Optimization

Booster High-level RF Frequency Tracking Improvement Via the Bias-Curve Optimization FERMILAB-TM-227-AD Booster High-level RF Frequency Tracking Improvement Via the Bias-Curve Optimization Xi Yang Fermi National Accelerator Laboratory Box 5, Batavia IL 651 Abstract It is important to improve

More information

MODERN AM BROADCAST STATIONS AM STEREO CQUAM WITH DDS

MODERN AM BROADCAST STATIONS AM STEREO CQUAM WITH DDS MODERN AM BROADCAST STATIONS AM STEREO CQUAM WITH DDS DDS EXCITER OPERATING MANUAL 20W CARRIER - 80W PEP WHAT IS DDS? IT IS THE INITIALS OF THE WORDS DIRECT DIGITAL SYNTHESIZER. THAT MEANS: DIRECT DIGITAL

More information

VALLIAMMAI ENGINEERING COLLEGE SRM Nagar, Kattankulathur-603 203 DEPARTMENT OF ELECTRONICS AND COMMUNICATION ENGINEERING EC6503 TRANSMISSION LINES AND WAVEGUIDES YEAR / SEMESTER: III / V ACADEMIC YEAR:

More information

GA A22574 ADVANTAGES OF TRAVELING WAVE RESONANT ANTENNAS FOR FAST WAVE HEATING SYSTEMS

GA A22574 ADVANTAGES OF TRAVELING WAVE RESONANT ANTENNAS FOR FAST WAVE HEATING SYSTEMS GA A22574 ADVANTAGES OF TRAVELING WAVE RESONANT ANTENNAS by D.A. PHELPS, F.W. BAITY, R.W. CALLIS, J.S. degrassie, C.P. MOELLER, and R.I. PINSKER APRIL 1997 This report was prepared as an account of work

More information

Module IV, Lecture 2 DNP experiments and hardware

Module IV, Lecture 2 DNP experiments and hardware Module IV, Lecture 2 DNP experiments and hardware tunnel diodes, Gunn diodes, magnetrons, traveling-wave tubes, klystrons, gyrotrons Dr Ilya Kuprov, University of Southampton, 2013 (for all lecture notes

More information

Acceleration 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 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 information

3 rd Harmonic Cavity at ELETTRA

3 rd Harmonic Cavity at ELETTRA 3 rd Harmonic Cavity at ELETTRA G.Penco, M.Svandrlik FERMI @ Elettra G.O.F. RF UPGRADE BOOSTER Big Projects Started FINALLY at ELETTRA during 25 Experiments with 3HC concluded in December 24 Now activities

More information

Converters for Cycling Machines

Converters for Cycling Machines Converters for Cycling Machines Neil Marks, DLS/CCLRC, Daresbury Laboratory, Warrington WA4 4AD, U.K. DC and AC accelerators; Contents suitable waveforms in cycling machines; the magnet load; reactive

More information

RF Cavity Design. Erk Jensen CERN BE/RF. CERN Accelerator School Accelerator Physics (Intermediate level) Darmstadt 2009

RF Cavity Design. Erk Jensen CERN BE/RF. CERN Accelerator School Accelerator Physics (Intermediate level) Darmstadt 2009 RF Cavity Design Erk Jensen CERN BE/RF CERN Accelerator School Accelerator Physics (Intermediate level) Darmstadt 009 CAS Darmstadt '09 RF Cavity Design 1 Overview DC versus RF Basic equations: Lorentz

More information

Design and RF Measurements of an X-band Accelerating Structure for the Sparc Project

Design and RF Measurements of an X-band Accelerating Structure for the Sparc Project Design and RF Measurements of an X-band Accelerating Structure for the Sparc Project INFN-LNF ; UNIVERSITY OF ROME LA SAPIENZA ; INFN - MI Presented by BRUNO SPATARO Erice, Sicily, October 9-14; 2005 SALAF

More information

Technician Licensing Class. Antennas

Technician Licensing Class. Antennas Technician Licensing Class Antennas Antennas A simple dipole mounted so the conductor is parallel to the Earth's surface is a horizontally polarized antenna. T9A3 Polarization is referenced to the Earth

More information

Candidate Design for a Multiband LMR Antenna System Using a Rudimentary Antenna Tuner

Candidate Design for a Multiband LMR Antenna System Using a Rudimentary Antenna Tuner Candidate Design for a Multiband LMR Antenna System Using a Rudimentary Antenna Tuner Steve Ellingson June 30, 2010 Contents 1 Introduction 3 2 Design Strategy 3 3 Candidate Design 8 4 Performance of Candidate

More information

Input Return Loss, db > 26 Narrowband to Narrowband Isolation, db > 30

Input Return Loss, db > 26 Narrowband to Narrowband Isolation, db > 30 Band III (VHF) TV Commutating Line Combiner 174-222 MHz CC VHF Series This style of circuit provides a relatively low cost combiner which is ideal, provided the frequency spacing is not too close. Compact,

More information