Geometrical and RF Considerations for All Beam Collisions via Crab- Crossing
|
|
- Hugh Terry
- 5 years ago
- Views:
Transcription
1 ARB Technical Note - raft - 1/7/97 Geometrical and RF Considerations for All Beam Collisions via Crab- Crossing Frank Zimmermann and avid H Whittum In this note we sketch the geometry for a crab-crossing scheme that achieves all beam collisions from a matrix linac, without temporal or spatial beam combining RF scalings are noted and appear not to present any challenges Clearly a more difficult idea should be found Geometry The matrix linac and one final focus scheme have been described in previous notes Here we consider the idea sketched in Fig1, of colliding beams at a crossing angle, θ The idea is that each bunch from N 5 parallel linacs, can be made to collide with each and every bunch of the opposing N 5 parallel linacs epth of focus, chromatic effects, and the effect of detector solenoidal field are issues; here we consider the zeroth order concerns: what angle is required for the matrix linac scheme, and what are rf requirements result for the crab cavities? nd Collision B L S θ θ 1st Collision FIGURE 1 Geometry for collision at crossing half-angle θ The geometrical relationships determining the required crossing angle are as follows: sin π θ = B S, (complementary angles) S = B +, (Theorem due to Pythagoras) L+ B=, (group delay in matrix transmission line) β g
2 Combining the first two relations, one finds S = sin θ, B= cot ( θ ) ( ) The third relation gives then the length travelled by the second bunch, to its collision point 1 L = cot ( θ) β g In order for the opposing bunch to arrive on time, we must have S = L, and thus we find 1 β g cot( θ)= csc ( θ), or tanθ = β g The current conceptual design for the matrix scheme uses β g, corresponding to θ rad For the sake of definiteness we fill in the other parameters, λ λ mm, 4 β g 5 5 λ λ 41 8 mm 4 The duration of one pulse of the N 5 parallel beam lines corresponds to N βg 6 5λ 15λ 5 41 mm 7 14 ns RF Considerations To accomodate the crossing angle without loss of luminosity, one would like to insure head on collisions This is to say that one would like the head of the beam entering from the left, in Fig 1, to pass through the head and the tail of the beam entering from the right This is illustrated in Fig, although not to scale (we are interested in beams of transverse extent σx σy nm, and bunch lengths long in comparison σ z 3 µ m)
3 θ FIGURE (a) When beams cross at an angle with no head-to-tail offset, the head ot the first bunch fails to collide with the tail of the second bunch θ FIGURE (b) When beams cross at an angle with the proper head-to-tail offset, the head ot the first bunch collides with the head and the tail of the second bunch, and all beam slices in between To accomplish head-on collisions, we must rotate the beam in the crossing plane We can see this as follows Let us suppose the head of bunch #1 follows the trajectory r h1 = t( cos θ,sinθ ), while the tail follows at approximately the same angle, but at an offset r = t T cos θ,sinθ r, ( )( )+ t1 t1 and we offset the time coordinate by T, to be determined For the oncoming bunch, bunch #, we have r h = t( cos θ,sinθ ), and r t = ( t T) ( cos θ,sinθ )+ r t Evidently the two heads collide at r r h1 = h = t= To insure that the tail of bunch #1 collides with the head of bunch #, we must have, for some t, r = t T cos θ,sinθ r r t cos θ,sinθ, ( )( )+ = = ( ) t1 t1 h
4 and we define this time to be t=t, so that r t1 = T( cos θ,sinθ ) Similarly then tail # should collide with head #1, r = t T cos θ,sinθ r r t cos θ,sinθ, ( )( )+ = = ( ) t t h1 and r t = T( cos θ,sinθ ) Thus the tail trajectories are parameterized according to r t1 = ( t T)( cos θ,sinθ)+ T( cos θ,sinθ)= ([ t T] cos θ, tsinθ ), r = ( t T) ( cos θ,sinθ)+ r = t+ T cos θ, tsinθ t t ([ ] ) Evidently the tails collide at t = T Treating T as a parameter of beam slices, one can see that each segment of the beam from the left, encounters each segment of the beam from the right, colliding at a point on the dashed centerline in Fig (b), at a point displaced vertically in the figure by an amount depending on the displacement of the slice from the beam head The offset r ( T)= T( cos θ,sin θ) ( T, Tθ ) amounts to a bunch rotation in the plane of the collision, and to accomplish this, we may present to the beam, a time varying deflection, x = α T, followed by transport (eg, a drift) x = R1x = R1α T For this to work we must require that x Tθ, and this determines the time-varying kick in terms of the crossing angle, θ α R1 For example, for a m drift, and a mrad crossing angle, one has α cm 1 At the same time we may relate α to RF parameters according to ε α = = = = T x px px e V T mcγ mc γ t mc γ x mc γ x Considering a standing-wave cavity, this voltage gradient may be related to power dissipated using the relations
5 R V x = / ωu, P diss ω Q U V/ x = = Q R / Q w w [ ] Thus, in terms of the transverse shunt impedance R Qw R / Q, V/ x = R P diss Conversely we may express power dissipated in terms of our kick parameter α, = [ ] P diss = Eα, R where E is the full beam voltage, 5 TV Equivalent voltage for our example is Eα 5 MV/cm Naturally we become interested in transverse shunt impedance at this point Since the voltage required is looking a bit large, high gradient may be required, and thus short-wavelength, planar structures would be of interest 1 Let us consider the case of a rectangular geometry consisting of a pillbox of transverse dimensions a b, and length L In this case, T 8Lβ x, β ab where the transit angle factor is ( ) sin θ / T =, ( θ / ) the transit angle θ = β L, and wavenumbers are βx = π / a,βy = π / b, β = βx + βy We may simplify this to read, x sin ( θ / ) 16 β ( ) ab θ / β Maximum occurs for θ=13356, corresponding to Q ab, 1+ a / b and for a 11 6 λ = b = λ/ (with λ the free-space wavelength) this may be expressed as 1 For the record, for a cylindrical pillbox of radius R, transit angle θ, sin ( θ / ) 39 1 ( θ / ) R avid H Whittum, ipole Mode eflection in the Subharmonic rive Experiment, ARB Technical Note 17
6 Wall quality factor takes the form 1 δ β β x y β = + + Q β a b L, w with the skin-depth δ = µ m/ f ( GHz) For our choice of aspect ratios this is λ Q w 181 δ The result for shunt impedance (for a single cavity) is then R Q R = w Z f 1 3/ 1 ( ) GHz MΩ / cm λδ If we couple N cavities together to be powered by a single feed, we may expect not quite N times the shunt impedance of a single cell (N/ if we do badly in the design) As an example, for a singe cell driven at 856 MHz, we find R 6 MΩ / cm If 1 cells were coupled into one single-feed standing wave structure, and derating the shunt impedance by a factor of, we would have 6MΩ/ cm, and 5 MV/cm P diss MΩ/ cm MW, (S-Band) comfortably less than the output of a SLE d SLAC 545 This scheme is actually a bit wasteful since the fill time for the structure would be 16 µs ( Q w ), much longer than the train of charge to be manipulated with the device At W-Band (9139 GHz) we find R 1 1 MΩ/ cm for one cell; for 1 cells, derated by a factor of two, we have 11 GΩ / cm Peak power required is then 6 kw, and the fill time is 9 ns ( Q w ), a good figure for a beam with this structure More Work The effect of synchrotron radiation in the course of the deflection by the cavities remains to be checked; it is a concern due to the large kick angle Aperture considerations and other wakefields sold separately Not valid after last date stamped Use only as directed o not ingest
Short Introduction to CLIC and CTF3, Technologies for Future Linear Colliders
Short Introduction to CLIC and CTF3, Technologies for Future Linear Colliders Explanation of the Basic Principles and Goals Visit to the CTF3 Installation Roger Ruber Collider History p p hadron collider
More informationRF LINACS. Alessandra Lombardi BE/ ABP CERN
1 RF LINACS Alessandra Lombardi BE/ ABP CERN Contents PART 1 (yesterday) : Introduction : why?,what?, how?, when? Building bloc I (1/) : Radio Frequency cavity From an RF cavity to an accelerator PART
More informationSuperconducting RF Accelerators: Why all the interest?
Superconducting RF Accelerators: Why all the interest? William A. Barletta Director, United States Particle Accelerator School Dept. of Physics, MIT The HEP prespective ILC PROJECT X Why do we need RF
More informationEmittance preservation in TESLA
Emittance preservation in TESLA R.Brinkmann Deutsches Elektronen-Synchrotron DESY,Hamburg, Germany V.Tsakanov Yerevan Physics Institute/CANDLE, Yerevan, Armenia The main approaches to the emittance preservation
More informationSLS at the Paul Scherrer Institute (PSI), Villigen, Switzerland
SLS at the Paul Scherrer Institute (PSI), Villigen, Switzerland Michael Böge 1 SLS Team at PSI Michael Böge 2 Layout of the SLS Linac, Transferlines Booster Storage Ring (SR) Beamlines and Insertion Devices
More informationLCLS S-band Structure Coupler
LCLS S-band Structure Coupler Zenghai Li Advanced Computations Department Stanford Linear Accelerator Center LCLS S-band L01/L02 Coupler Review Nov. 03, 2004 Overview Motivation Modeling tools Multipole
More informationTeV Scale Muon RLA Complex Large Emittance MC Scenario
TeV Scale Muon RLA Complex Large Emittance MC Scenario Alex Bogacz and Kevin Beard Muon Collider Design Workshop, BNL, December 1-3, 29 Outline Large Emittance MC Neuffer s Collider Acceleration Scheme
More informationBeam-beam Effects in Linear Colliders
Beam-beam Effects in Linear Colliders Daniel Schulte D. Schulte Beam-beam effects in Linear Colliders 1 Generic Linear Collider Single pass poses luminosity challenge Low emittances are produced in the
More informationDiagnostic Systems for Characterizing Electron Sources at the Photo Injector Test Facility at DESY, Zeuthen site
1 Diagnostic Systems for Characterizing Electron Sources at the Photo Injector Test Facility at DESY, Zeuthen site Sakhorn Rimjaem (on behalf of the PITZ team) Motivation Photo Injector Test Facility at
More informationX-Band RF Harmonic Compensation for Linear Bunch Compression in the LCLS
SLAC-TN-5- LCLS-TN-1-1 November 1,1 X-Band RF Harmonic Compensation for Linear Bunch Compression in the LCLS Paul Emma SLAC November 1, 1 ABSTRACT An X-band th harmonic RF section is used to linearize
More informationTools of Particle Physics I Accelerators
Tools of Particle Physics I Accelerators W.S. Graves July, 2011 MIT W.S. Graves July, 2011 1.Introduction to Accelerator Physics 2.Three Big Machines Large Hadron Collider (LHC) International Linear Collider
More informationDesign of an RF Photo-Gun (PHIN)
Design of an RF Photo-Gun (PHIN) R. Roux 1, G. Bienvenu 1, C. Prevost 1, B. Mercier 1 1) CNRS-IN2P3-LAL, Orsay, France Abstract In this note we show the results of the RF simulations performed with a 2-D
More informationStatus of linear collider designs:
Status of linear collider designs: Main linacs Design overview, principal open issues G. Dugan March 11, 2002 Linear colliders: main linacs The main linac is the heart of the linear collider TESLA, NLC/JLC,
More informationLecture 1 Introduction to RF for Accelerators. Dr G Burt Lancaster University Engineering
Lecture 1 Introduction to RF for Accelerators Dr G Burt Lancaster University Engineering Electrostatic Acceleration + - - - - - - - + + + + + + Van-de Graaff - 1930s A standard electrostatic accelerator
More informationAccelerator Physics Final Exam pts.
Accelerator Physics Final Exam - 170 pts. S. M. Lund and Y. Hao Graders: C. Richard and C. Y. Wong June 14, 2018 Problem 1 P052 Emittance Evolution 40 pts. a) 5 pts: Consider a coasting beam composed of
More informationCERN Accelerator School. RF Cavities. Erk Jensen CERN BE-RF
CERN Accelerator School RF Cavities Erk Jensen CERN BE-RF CERN Accelerator School, Varna 010 - "Introduction to Accelerator Physics" What is a cavity? 3-Sept-010 CAS Varna/Bulgaria 010- RF Cavities Lorentz
More information6 Bunch Compressor and Transfer to Main Linac
II-159 6 Bunch Compressor and Transfer to Main Linac 6.1 Introduction The equilibrium bunch length in the damping ring (DR) is 6 mm, too long by an order of magnitude for optimum collider performance (σ
More informationFundamental Concepts of Particle Accelerators III : High-Energy Beam Dynamics (2) Koji TAKATA KEK. Accelerator Course, Sokendai. Second Term, JFY2012
.... Fundamental Concepts of Particle Accelerators III : High-Energy Beam Dynamics (2) Koji TAKATA KEK koji.takata@kek.jp http://research.kek.jp/people/takata/home.html Accelerator Course, Sokendai Second
More informationUpstream Polarimetry with 4-Magnet Chicane
2005 International Linear Collider Workshop Stanford, U.S.A. Upstream Polarimetry with 4-Magnet Chicane N. Meyners, V. Gharibyan, K.P. Schüler DESY, Hamburg, Germany We have extended an earlier polarimeter
More informationTraveling Wave Undulators for FELs and Synchrotron Radiation Sources
LCLS-TN-05-8 Traveling Wave Undulators for FELs and Synchrotron Radiation Sources 1. Introduction C. Pellegrini, Department of Physics and Astronomy, UCLA 1 February 4, 2005 We study the use of a traveling
More informationIntroduction to accelerators for teachers (Korean program) Mariusz Sapiński CERN, Beams Department August 9 th, 2012
Introduction to accelerators for teachers (Korean program) Mariusz Sapiński (mariusz.sapinski@cern.ch) CERN, Beams Department August 9 th, 2012 Definition (Britannica) Particle accelerator: A device producing
More informationAccelerator Physics Issues of ERL Prototype
Accelerator Physics Issues of ERL Prototype Ivan Bazarov, Geoffrey Krafft Cornell University TJNAF ERL site visit (Mar 7-8, ) Part I (Bazarov). Optics. Space Charge Emittance Compensation in the Injector
More informationWakefield computations for the LCLS Injector (Part I) *
LCLS-TN-05-17 Wakefield computations for the LCLS Injector (Part I) * June 13 th 005 (reedited May 007) C.Limborg-Deprey, K.Bane Abstract In this document, we report on basic wakefield computations used
More information$)ODW%HDP(OHFWURQ6RXUFHIRU/LQHDU&ROOLGHUV
$)ODW%HDP(OHFWURQ6RXUFHIRU/LQHDU&ROOLGHUV R. Brinkmann, Ya. Derbenev and K. Flöttmann, DESY April 1999 $EVWUDFW We discuss the possibility of generating a low-emittance flat (ε y
More informationLinac JUAS lecture summary
Linac JUAS lecture summary Part1: Introduction to Linacs Linac is the acronym for Linear accelerator, a device where charged particles acquire energy moving on a linear path. There are more than 20 000
More informationNovel Features of Computational EM and Particle-in-Cell Simulations. Shahid Ahmed. Illinois Institute of Technology
Novel Features of Computational EM and Particle-in-Cell Simulations Shahid Ahmed Illinois Institute of Technology Outline Part-I EM Structure Motivation Method Modes, Radiation Leakage and HOM Damper Conclusions
More informationPhysics 610. Adv Particle Physics. April 7, 2014
Physics 610 Adv Particle Physics April 7, 2014 Accelerators History Two Principles Electrostatic Cockcroft-Walton Van de Graaff and tandem Van de Graaff Transformers Cyclotron Betatron Linear Induction
More informationLinear Collider Collaboration Tech Notes
LCC-0073 SLAC-PUB-9004 September 2001 Linear Collider Collaboration Tech Notes Microwave Quadrupoles for Beam Break-up Supression In the NLC Main Linac K.L.F. Bane and G. Stupakov Stanford Linear Accelerator
More informationImpedance & Instabilities
Impedance & Instabilities The concept of wakefields and impedance Wakefield effects and their relation to important beam parameters Beam-pipe geometry and materials and their impact on impedance An introduction
More informationThe Booster has three magnet systems for extraction: Kicker Ke, comprising two identical magnets and power supplies Septum Se
3.2.7 Booster Injection and Extraction 3.2.7.1 Overview The Booster has two magnet systems for injection: Septum Si Kicker Ki The Booster has three magnet systems for extraction: Kicker Ke, comprising
More information1.5-GeV FFAG Accelerator as Injector to the BNL-AGS
1.5-GeV FFAG Accelerator as Injector to the BNL-AGS Alessandro G. Ruggiero M. Blaskiewicz,, T. Roser, D. Trbojevic,, N. Tsoupas,, W. Zhang Oral Contribution to EPAC 04. July 5-9, 5 2004 Present BNL - AGS
More informationIntroduction to Collider Physics
Introduction to Collider Physics William Barletta United States Particle Accelerator School Dept. of Physics, MIT The Very Big Picture Accelerators Figure of Merit 1: Accelerator energy ==> energy frontier
More informationLinear Collider Collaboration Tech Notes. Design Studies of Positron Collection for the NLC
LCC-7 August 21 Linear Collider Collaboration Tech Notes Design Studies of Positron Collection for the NLC Yuri K. Batygin, Ninod K. Bharadwaj, David C. Schultz,John C. Sheppard Stanford Linear Accelerator
More informationLCLS Injector Prototyping at the GTF
LCLS Injector Prototyping at at the GTF John John Schmerge, SLAC SLAC November 3, 3, 23 23 GTF GTF Description Summary of of Previous Measurements Longitudinal Emittance Transverse Emittance Active LCLS
More informationLetter of Intent for KEK Super B Factory
Letter of Intent for KEK Super B Factory Part III: Accelerator Design edited by J. W. Flanagan and Y. Ohnishi August 9, 2004 Contents Executive Summary 341 1 Machine Parameters 344 1.1 Luminosity...................................
More informationFrequency and time domain analysis of trapped modes in the CERN Proton Synchrotron
Frequency and time domain analysis of trapped modes in the CERN Proton Synchrotron Serena Persichelli CERN Impedance and collective effects BE-ABP-ICE Abstract The term trapped mode refers to a resonance
More informationTHz Electron Gun Development. Emilio Nanni 3/30/2016
THz Electron Gun Development Emilio Nanni 3/30/2016 Outline Motivation Experimental Demonstration of THz Acceleration THz Generation Accelerating Structure and Results Moving Forward Parametric THz Amplifiers
More informationSpeculations About a Fourier Series Kicker for the TESLA Damping Ring
1 Speculations About a Fourier Series Kicker for the TESLA Damping Ring George D. Gollin *, Thomas R. Junk Dept. of Physics, University of Illinois at Urbana-Champaign, Urbana, IL 61801 August 28, 2002
More informationBuilding block. sources: paracle species + intensity (charge) acceleraaon process: energy & intensity
Building block sources: paracle species + intensity (charge) acceleraaon process: energy & intensity pre- accelerator (someame): boost paracle energy for injecaon in accelerator front- end use: target,
More informationBeam Shaping and Permanent Magnet Quadrupole Focusing with Applications to the Plasma Wakefield Accelerator
Beam Shaping and Permanent Magnet Quadrupole Focusing with Applications to the Plasma Wakefield Accelerator R. Joel England J. B. Rosenzweig, G. Travish, A. Doyuran, O. Williams, B. O Shea UCLA Department
More informationDielectric Accelerators at CLARA. G. Burt, Lancaster University On behalf of ASTeC, Lancaster U., Liverpool U., U. Manchester, and Oxford U.
Dielectric Accelerators at CLARA G. Burt, Lancaster University On behalf of ASTeC, Lancaster U., Liverpool U., U. Manchester, and Oxford U. Dielectric Accelerators Types Photonic structures Dielectric
More informationSimulations for photoinjectors C.Limborg
Simulations for photoinjectors C.Limborg 1- GTF Simulations Parmela modeling improvements Comparison to experimental results: 2ps & 4ps Sensitivity study Plans for future simulations 2- LCLS Injector Simulations
More informationFemto second X ray Pulse Generation by Electron Beam Slicing. F. Willeke, L.H. Yu, NSLSII, BNL, Upton, NY 11973, USA
Femto second X ray Pulse Generation by Electron Beam Slicing F. Willeke, L.H. Yu, NSLSII, BNL, Upton, NY 11973, USA r 2 r 1 y d x z v Basic Idea: When short electron bunch from linac (5MeV, 50pC,100fs)
More informationSBF Accelerator Principles
SBF Accelerator Principles John Seeman SLAC Frascati Workshop November 11, 2005 Topics The Collision Point Design constraints going backwards Design constraints going forward Parameter relations Luminosity
More informationWakefield Effects of Collimators in LCLS-II
Wakefield Effects of Collimators in LCLS-II LCLS-II TN-15-38 10/7/2015 K. Bane SLAC, Menlo Park, CA 94025, USA October 7, 2015 LCLSII-TN-15-38 L C L S - I I T E C H N I C A L N O T E LCLS-TN-15-38 October
More informationANALYSIS OF HIGH ORDER MODES IN 1.3 GHZ CW SRF ELECTRON LINAC FOR A LIGHT SOURCE
ANALYSIS OF HIGH ORDER MODES IN 1.3 GHZ CW SRF ELECTRON LINAC FOR A LIGHT SOURCE A. Sukhanov, A. Vostrikov, V. Yakovlev, Fermilab, Batavia, IL 60510, USA Abstract Design of a Light Source (LS) based on
More informationAlignment requirement for the SRF cavities of the LCLS-II injector LCLSII-TN /16/2014
Alignment requirement for the SRF cavities of the LCLS-II injector LCLS-II TN-14-16 12/16/2014 R. K. Li, C. Papadopoulos, T. O. Raubenheimer, J. F. Schmerge, and F. Zhou December 16, 2014 LCLSII-TN-14-16
More informationAccelerator Physics. Tip World Scientific NEW JERSEY LONDON SINGAPORE BEIJING SHANGHAI HONG KONG TAIPEI BANGALORE. Second Edition. S. Y.
Accelerator Physics Second Edition S. Y. Lee Department of Physics, Indiana University Tip World Scientific NEW JERSEY LONDON SINGAPORE BEIJING SHANGHAI HONG KONG TAIPEI BANGALORE Contents Preface Preface
More informationILC Particle Sources -Electron and PositronMasao KURIKI (Hiroshima University)
ILC Particle Sources -Electron and PositronMasao KURIKI (Hiroshima University) Introduction Electron Polarization is important for ILC. NEA GaAs is practically the only solution. Positron polarization
More informationHigh-Gradient, Millimeter Wave Accelerating Structure
DPF2015-337 August 31, 2015 High-Gradient, Millimeter Wave Accelerating Structure S.V. Kuzikov 1,2, A.A. Vikharev 1,3, N.Yu. Peskov 1 1 Institute of Applied Physics, 46 Ulyanova Str., Nizhny Novgorod,
More informationThe Relativistic Stern-Gerlach Interaction as a Tool for Attaining the Spin Separation
The Relativistic Stern-Gerlach Interaction as a Tool for Attaining the Spin Separation P. Cameron, M. Conte, A. U. Luccio, W. W. MacKay, M. Palazzi and M. Pusterla Brookhaven National Laboratory, Upton,
More informationUse of Crab Cavities for Short X-ray Pulse Production in Rings
Use of Crab Cavities for Short X-ray Pulse Production in Rings Michael Borland Argonne National Laboratory March 2010 The submitted manuscript has been created by UChicago Argonne, LLC, Operator of Argonne
More informationCEPC and FCCee parameters from the viewpoint of the beam-beam and electron cloud effects. K. Ohmi (KEK) IAS-HEP, HKUST, Hong Kong Jan.
CEPC and FCCee parameters from the viewpoint of the beam-beam and electron cloud effects K. Ohmi (KEK) IAS-HEP, HKUST, Hong Kong Jan. 22-25, 2018 CEPC Parameters Y. Zhang, CEPC conference Nov. 2017, IHEP
More informationExperimental Optimization of Electron Beams for Generating THz CTR and CDR with PITZ
Experimental Optimization of Electron Beams for Generating THz CTR and CDR with PITZ Introduction Outline Optimization of Electron Beams Calculations of CTR/CDR Pulse Energy Summary & Outlook Prach Boonpornprasert
More informationParticle physics experiments
Particle physics experiments Particle physics experiments: collide particles to produce new particles reveal their internal structure and laws of their interactions by observing regularities, measuring
More informationCERN Accelerator School. Intermediate Accelerator Physics Course Chios, Greece, September Low Emittance Rings
CERN Accelerator School Intermediate Accelerator Physics Course Chios, Greece, September 2011 Low Emittance Rings Part 1: Beam Dynamics with Synchrotron Radiation Andy Wolski The Cockcroft Institute, and
More informationASTRA simulations of the slice longitudinal momentum spread along the beamline for PITZ
ASTRA simulations of the slice longitudinal momentum spread along the beamline for PITZ Orlova Ksenia Lomonosov Moscow State University GSP-, Leninskie Gory, Moscow, 11999, Russian Federation Email: ks13orl@list.ru
More informationELIC Design. Center for Advanced Studies of Accelerators. Jefferson Lab. Second Electron-Ion Collider Workshop Jefferson Lab March 15-17, 2004
ELIC Design Ya. Derbenev, K. Beard, S. Chattopadhyay, J. Delayen, J. Grames, A. Hutton, G. Krafft, R. Li, L. Merminga, M. Poelker, E. Pozdeyev, B. Yunn, Y. Zhang Center for Advanced Studies of Accelerators
More informationCompressor Ring. Contents Where do we go? Beam physics limitations Possible Compressor ring choices Conclusions. Valeri Lebedev.
Compressor Ring Valeri Lebedev Fermilab Contents Where do we go? Beam physics limitations Possible Compressor ring choices Conclusions Muon Collider Workshop Newport News, VA Dec. 8-1, 8 Where do we go?
More informationEFFECTS OF RF DEFLECTIONS ON BEAM DYNAMICS IN LINEAR COLLIDERS*
SLAC-PUB-5069 September 1989 09 EFFECTS OF RF DEFLECTIONS ON BEAM DYNAMICS IN LINEAR COLLIDERS* J. T. SEEMAN Stanford Linear Accelerator Center, Stanford University, Stanford, CA 94309. Abstract The beam
More informationThe MAX IV Thermionic preinjector
The MAX IV Thermionic preinjector David Olsson ESLS RF, Lund, 2015-09-30 Injection Requirements I Full-energy injection from the LINAC 1.5 GeV and 3 GeV extraction points. Both storage rings will be operated
More informationPractical Lattice Design
Practical Lattice Design Dario Pellegrini (CERN) dario.pellegrini@cern.ch USPAS January, 15-19, 2018 1/17 D. Pellegrini - Practical Lattice Design Lecture 5. Low Beta Insertions 2/17 D. Pellegrini - Practical
More informationAccelerator R&D Opportunities: Sources and Linac. Developing expertise. D. Rubin, Cornell University
Accelerator R&D Opportunities: Sources and Linac D. Rubin, Cornell University Electron and positron sources Requirements Status of R&D Linac Modeling of beam dynamics Development of diagnostic and tuning
More informationStudies of trapped modes in the new extraction septum of the CERN Proton Synchrotron
Studies of trapped modes in the new extraction septum of the CERN Proton Synchrotron Serena Persichelli CERN Impedance and collective effects (BE-ABP-ICE) LIU LHC Injectors Upgrade project Università di
More informationINSTABILITIES IN LINACS. Massimo Ferrario INFN-LNF
INSTABILITIES IN LINACS Massimo Ferrario INFN-LNF Trondheim, 4 August, 13 SELF FIELDS AND WAKE FIELDS Direct self fields Image self fields Space Charge Wake fields γ = 1 1 β E = q 4πε o ( 1 β ) ( 1 β sin
More informationEstimates of local heating due to trapped modes in vacuum chamber
Estimates of local heating due to trapped modes in vacuum chamber Gennady Stupakov SLAC National Accelerator Laboratory, Menlo Park, CA 94025 CERN, April 29, 2016 2 Motivation The motivation for this analysis
More informationSPARCLAB. Source For Plasma Accelerators and Radiation Compton. On behalf of SPARCLAB collaboration
SPARCLAB Source For Plasma Accelerators and Radiation Compton with Laser And Beam On behalf of SPARCLAB collaboration EMITTANCE X X X X X X X X 2 BRIGHTNESS (electrons) B n 2I nx ny A m 2 rad 2 The current
More informationHELICAL COOLING CHANNEL PROGRESS*
Muons, Inc. HELICAL COOLING CHANNEL PROGRESS* R. P. Johnson #, Muons, Inc., Batavia, IL, U.S.A. Y. S. Derbenev, JLab, Newport News, VA, USA K. Yonehara, Fermilab, Batavia, IL, USA (and many other SBIR-STTR
More informationThe 2015 erhic Ring-Ring Design. Christoph Montag Collider-Accelerator Department Brookhaven National Laboratory
The 2015 erhic Ring-Ring Design Christoph Montag Collider-Accelerator Department Brookhaven National Laboratory The Relativistic Heavy Ion Collider RHIC Two superconducting storage rings 3833.845 m circumference
More informationCalculation of Wakefields and Higher Order Modes for the New Design of the Vacuum Chamber of the ALICE Experiment for the HL-LHC
CERN-ACC-NOTE-2017-0033 23rd May 2017 rainer.wanzenberg@desy.de Calculation of Wakefields and Higher Order Modes for the New Design of the Vacuum Chamber of the ALICE Experiment for the HL-LHC R. Wanzenberg
More informationLow energy electron storage ring with tunable compaction factor
REVIEW OF SCIENTIFIC INSTRUMENTS 78, 075107 2007 Low energy electron storage ring with tunable compaction factor S. Y. Lee, J. Kolski, Z. Liu, X. Pang, C. Park, W. Tam, and F. Wang Department of Physics,
More informationLecture 5: Photoinjector Technology. J. Rosenzweig UCLA Dept. of Physics & Astronomy USPAS, 7/1/04
Lecture 5: Photoinjector Technology J. Rosenzweig UCLA Dept. of Physics & Astronomy USPAS, 7/1/04 Technologies Magnetostatic devices Computational modeling Map generation RF cavities 2 cell devices Multicell
More informationBeam Physics at SLAC. Yunhai Cai Beam Physics Department Head. July 8, 2008 SLAC Annual Program Review Page 1
Beam Physics at SLAC Yunhai Cai Beam Physics Department Head July 8, 2008 SLAC Annual Program Review Page 1 Members in the ABP Department * Head: Yunhai Cai * Staff: Gennady Stupakov Karl Bane Zhirong
More informationBERLinPro. An ERL Demonstration facility at the HELMHOLTZ ZENTRUM BERLIN
BERLinPro An ERL Demonstration facility at the HELMHOLTZ ZENTRUM BERLIN BERLinPro: ERL demonstration facility to prepare the ground for a few GeV ERL @ Berlin-Adlershof Goal: 100MeV, 100mA beam Small emittance,
More informationThomX Machine Advisory Committee. (LAL Orsay, March ) Ring Beam Dynamics
ThomX Machine Advisory Committee (LAL Orsay, March 20-21 2017) Ring Beam Dynamics A. Loulergue, M. Biagini, C. Bruni, I. Chaikovska I. Debrot, N. Delerue, A. Gamelin, H. Guler, J. Zang Programme Investissements
More informationLinear Collider Collaboration Tech Notes
LCC 0035 07/01/00 Linear Collider Collaboration Tech Notes More Options for the NLC Bunch Compressors January 7, 2000 Paul Emma Stanford Linear Accelerator Center Stanford, CA Abstract: The present bunch
More informationLow Emittance Machines
Advanced Accelerator Physics Course RHUL, Egham, UK September 2017 Low Emittance Machines Part 1: Beam Dynamics with Synchrotron Radiation Andy Wolski The Cockcroft Institute, and the University of Liverpool,
More informationLab Report TEMF - TU Darmstadt
Institut für Theorie Elektromagnetischer Felder Lab Report TEMF - TU Darmstadt W. Ackermann, R. Hampel, M. Kunze T. Lau, W.F.O. Müller, S. Setzer, T. Weiland, I. Zagorodnov TESLA Collaboration Meeting
More informationWakefield induced Losses in the Manual Valves of the TESLA Cryomodule
Wakefield induced Losses in the Manual Valves of the TESLA Cryomodule Abstract M. Dohlus, H.-P. Wedekind, K. Zapfe Deutsches Elektronen Synchrotron Notkestr. 85, D-22603 Hamburg, Germany The beam pipe
More informationThe High Power Electrodynamics Group at Los Alamos National Laboratory
The High Power Electrodynamics Group at Los Alamos National Laboratory Steven J. Russell Los Alamos National Laboratory Slide 1 Los Alamos National Laboratory Valles Caldera Los Alamos Slide 2 Los Alamos
More informationSTATUS OF E-157: METER-LONG PLASMA WAKEFIELD EXPERIMENT. Presented by Patrick Muggli for the E-157 SLAC/USC/LBNL/UCLA Collaboration
STATUS OF E-157: METER-LONG PLASMA WAKEFIELD EXPERIMENT Presented by Patrick Muggli for the E-157 SLAC/USC/LBNL/UCLA Collaboration OUTLINE Basic E-157 Acelleration, Focusing Plasma Source Diagnostics:
More informationSingle-Bunch Effects from SPX Deflecting Cavities
Single-Bunch Effects from SPX Deflecting Cavities Yong-Chul Chae and Louis Emery Accelerator Operation Group Accelerator System Division Measurements March 13, 2013 Introduction The single bunch current
More informationA Two-Stage Bunch Compressor Option for the US Cold LC
LCC-0151 SLAC-TN-0-048 June 2004 Linear Collider Collaboration Tech Notes A Two-Stage Bunch Compressor Option for the US Cold LC Abstract This note documents a set of expressions used to explore the issue
More informationPreliminary design study of JUICE. Joint Universities International Circular Electronsynchrotron
Preliminary design study of JUICE Joint Universities International Circular Electronsynchrotron Goal Make a 3th generation Synchrotron Radiation Lightsource at 3 GeV Goal Make a 3th generation Synchrotron
More informationAngular momentum dominated electron beam and flat beam generation. FNPL video conference Feb. 28, 2005 Yin-e Sun 1
Angular momentum dominated electron beam and flat beam generation yinesun@uchicago.edu FNPL video conference Feb. 8, 5 Yin-e Sun 1 outline angular momentum dominated electron beam and its applications
More informationPhysics 736. Experimental Methods in Nuclear-, Particle-, and Astrophysics. - Accelerator Techniques: Introduction and History -
Physics 736 Experimental Methods in Nuclear-, Particle-, and Astrophysics - Accelerator Techniques: Introduction and History - Karsten Heeger heeger@wisc.edu Homework #8 Karsten Heeger, Univ. of Wisconsin
More informationX-band Experience at FEL
X-band Experience at FERMI@Elettra FEL Gerardo D Auria Elettra - Sincrotrone Trieste GdA_TIARA Workshop, Ångström Laboratory, June 17-19, 2013 1 Outline The FERMI@Elettra FEL project Machine layout and
More informationTransverse dynamics Selected topics. Erik Adli, University of Oslo, August 2016, v2.21
Transverse dynamics Selected topics Erik Adli, University of Oslo, August 2016, Erik.Adli@fys.uio.no, v2.21 Dispersion So far, we have studied particles with reference momentum p = p 0. A dipole field
More informationStart-to-End Simulations
AKBP 9.3 Case Study for 100 µm SASE FEL Based on PITZ Accelerator for Pump-Probe Experiment at the European XFEL Start-to-End Simulations Outline Introduction Beam Optimization Beam Transport Simulation
More informationSimulations of the IR/THz source at PITZ (SASE FEL and CTR)
Simulations of the IR/THz source at PITZ (SASE FEL and CTR) Introduction Outline Simulations of SASE FEL Simulations of CTR Summary Issues for Discussion Mini-Workshop on THz Option at PITZ DESY, Zeuthen
More information( ( )) + w ( ) 3 / 2
K K DA!NE TECHNICAL NOTE INFN - LNF, Accelerator Division Frascati, March 4, 1 Note: G-7 SYNCHROTRON TUNE SHIFT AND TUNE SPREAD DUE TO BEAM-BEAM COLLISIONS WITH A CROSSING ANGLE M. Zobov and D. Shatilov
More informationStatus of Optics Design
17th B2GM, February 5, 2014 Status of Optics Design Y. Ohnishi /KEK 17th B2GM KEK, February 5, 2014 Contents! Lattice parameters! Dynamic aperture under influence of beam-beam effect! Lattice preparation
More informationH. Maesaka*, H. Ego, T. Hara, A. Higashiya, S. Inoue, S. Matsubara, T. Ohshima, K. Tamasaku, H. Tanaka, T. Tanikawa, T. Togashi, K. Togawa, H.
H. Maesaka*, H. Ego, T. Hara, A. Higashiya, S. Inoue, S. Matsubara, T. Ohshima, K. Tamasaku, H. Tanaka, T. Tanikawa, T. Togashi, K. Togawa, H. Tomizawa, M. Yabashi, K. Yanagida, T. Shintake and Y. Otake
More informationAn Introduction to Particle Accelerators. v short
An Introduction to Particle Accelerators v1.42 - short LHC FIRST BEAM 10-sep-2008 Introduction Part 1 Particle accelerators for HEP LHC: the world biggest accelerator, both in energy and size (as big as
More informationFirst Collective Effects Measurements in NSLS-II A. Blednykh Accelerator Physicist, BNL/NSLS-II Sep , 2014
First Collective Effects Measurements in NSLS-II A. Blednykh Accelerator Physicist, BNL/NSLS-II Sep. 17-19, 2014 (LOWεRING 2014) 1 BROOKHAVEN SCIENCE ASSOCIATES Outline Phase 1 (25mA / PETRA-III) and Phase
More informationDIAGNOSTIC TEST-BEAM-LINE FOR THE MESA INJECTOR
DIAGNOSTIC TEST-BEAM-LINE FOR THE MESA INJECTOR I.Alexander,K.Aulenbacher,V.Bechthold,B.Ledroit,C.Matejcek InstitutfürKernphysik,JohannesGutenberg-Universität,D-55099Mainz,Germany Abstract With the test-beam-line
More informationIntroduction to particle accelerators
Introduction to particle accelerators Walter Scandale CERN - AT department Lecce, 17 June 2006 Introductory remarks Particle accelerators are black boxes producing either flux of particles impinging on
More informationVarying accelerating fields
Varying accelerating fields Two approaches for accelerating with time-varying fields Linear Accelerators Circular Accelerators Use many accelerating cavities through which the particle beam passes once.
More informationILC Beam Dynamics Studies Using PLACET
ILC Beam Dynamics Studies Using PLACET Andrea Latina (CERN) July 11, 2007 John Adams Institute for Accelerator Science - Oxford (UK) Introduction Simulations Results Conclusions and Outlook PLACET Physical
More informationLattice Design and Performance for PEP-X Light Source
Lattice Design and Performance for PEP-X Light Source Yuri Nosochkov SLAC National Accelerator Laboratory With contributions by M-H. Wang, Y. Cai, X. Huang, K. Bane 48th ICFA Advanced Beam Dynamics Workshop
More information