CW Linac: Optics with Quads or Doublets. N. Perunov and N.Solyak Nov.6, 2009.

Slides:



Advertisements
Similar presentations
MEBT Design Considerations The beam energy in the MEBT is sufficiently low for the space charge forces to have a considerable impact on the beam dynamics.
Advertisements

A Capture Section Design for the CLIC Positron Source A. VIVOLI* Thanks to: L. RINOLFI (CERN) R. CHEHAB (IPNL & LAL / IN2P3-CNRS) O. DADOUN, P. LEPERCQ,
Emittance dilution due to misalignment of quads and cavities of ILC main linac revised K.Kubo For beam energy 250 GeV,
R. Miyamoto, Beam Physics Design of MEBT, ESS AD Retreat 1 Beam Physics Design of MEBT Ryoichi Miyamoto (ESS) November 29th, 2012 ESS AD Retreat On behalf.
Emittance dilution due to misalignment of quads and cavities of ILC main linac K.Kubo For beam energy 250 GeV, TESLA-type optics for 24MV/m.
Eric Prebys, FNAL.  So far, we’ve talked about nice, periodic lattice, but that may not be all that useful in the real world. In particular, we generally.
Electron Model Components and Costing C. Johnstone Summary talk, C. Johnstone FFAG04 Oct 12-16, 2004 KEK, Tsukuba, Japan.
Cryomodule Quad Doublet Solutions – M Church 9/12/07 1 NML Cryomodule Quad Doublet Lattice Solutions  Question  Are quadrupoles required as part of the.
SuperB Damping Rings M. Biagini, LNF-INFN P. Raimondi, SLAC/INFN A. Wolski, Cockroft Institute, UK SuperB III Workshop, SLAC, June 2006.
Simulated real beam into simulated MICE1 Mark Rayner CM26.
Recirculating pass optics V.Ptitsyn, D.Trbojevic, N.Tsoupas.
Preliminary result on Quarter wave transformer simulation a short lens with a high magnetic field and a long solenoidal magnetic field. Field profile of.
November 2005M. Woodley1 ILC Beam Delivery System layout with end-of-linac undulator.
ILC RTML Lattice Design A.Vivoli, N. Solyak, V. Kapin Fermilab.
Ajit Kurup, C. Bontoiu, M. Aslaninejad, J. Pozimski, Imperial College London. A.Bogacz, V. S. Morozov, Y.R. Roblin Jefferson Laboratory K. B. Beard, Muons,
Page 1 Review 09/2010 MEIC Ion Linac and Pre-Booster Design Bela Erdelyi Department of Physics, Northern Illinois University, and Physics Division, Argonne.
~ gun3.9 GHz cavity Bunch compressor 3 ILC cryomodules 45 deg. spectro injector main linac user area disp. area transport line Overview of.
Operated by JSA for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility EIC Collaboration Meeting, Hampton University, May 19-23,
Operated by the Jefferson Science Associates for the U.S. Depart. Of Energy Thomas Jefferson National Accelerator Facility Alex Bogacz, Dogbone RLA – Design.
Eric Prebys, FNAL.  In our previous discussion, we implicitly assumed that the distribution of particles in phase space followed the ellipse defined.
Project X Injector Experiment (PXIE) Sergei Nagaitsev Dec 19, 2011.
Positron source beamline lattice Wanming Liu, ANL
Module 5 A quick overview of beam dynamics in linear accelerators
Status of RTML design in TDR configuration A.Vivoli, N. Solyak, V. Kapin Fermilab.
Operated by the Southeastern Universities Research Association for the U.S. Depart. Of Energy Thomas Jefferson National Accelerator Facility Alex Bogacz,
A.Saini, K.Ranjan, N.Solyak, S.Mishra, V.Yakovlev on the behalf of our team Feb. 8, 2011 Study of failure effects of elements in beam transport line &
Project X: Accelerators Sergei Nagaitsev September 2, 2011.
LCLS-II Injector layout design and study Feng Zhou 8/19/2015.
CW Linac (ICD-2+): Lattice Design in Project-X, Nikolay Solyak (on behalf of team: F.Ostiguy, J-P.Carneiro, N.Perunov, A.Vostrikov, A.Saini, V.Yakovlev,
Operated by JSA for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility Alex Bogacz Status and Plans for Linac and RLAs.
Linac Design: Single-Spoke Cavities.
Finalising Oct’14 eRHIC lattices Including low-energy ring October 27, 2014Stephen Brooks, eRHIC FFAG meeting1.
Beam dynamics and linac optics studies for medical proton accelerators
CW Linac Lattice August, 29 N.Solyak, B.Shteynas.
Choppers Comparison of three schemes of choppers is made 2.5 MeV and 2.1 MeV beam energies are considered Presented by Boris Shteynas May,
Operated by the Jefferson Science Associates for the U.S. Depart. Of Energy Thomas Jefferson National Accelerator Facility Alex Bogacz, Acceleration in.
Operated by JSA for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility Alex Bogacz IDS- NF Acceleration Meeting, Jefferson Lab,
Overview of the RISP SCL
Arun Saini, N. Solyak Fermi National Accelerator Laboratory
General Design of C-ADS Accelerator Physics
eRHIC FFAG Lattice Design
Physics design on the main linac
SC Quadrupole Magnets in ILC Cryomodules
Large Booster and Collider Ring
Alternate Lattice for LCLS-II LTU Y
AD & I : BDS Lattice Design Changes
Limitations of Electron Beam Conditioning in Free-Electron Lasers
Muon Inverse Rotation and Acceleration
Progress of SPPC lattice design
LHC (SSC) Byung Yunn CASA.
Pulsed Ion Linac for EIC
Collider Ring Optics & Related Issues
MEBT1&2 design study for C-ADS
Negative Momentum Compaction lattice options for PS2
Comparison of NMC rings for PS2
Studies on orbit corrections
DTL M. Comunian M. Eshraqi.
PS2 meeting NMC lattice for PS2 Y. Papaphilippou September 28th, 2007.
Towards an NMC Ring: Dispersion suppressor & long straight section
Optics considerations for PS2
Crab crossing plan Optimize the crabbing system for best beam stability and minimum emittance impact Study and specify tolerances on cavity multipole components.
Towards an NMC Ring: Dispersion suppressor & long straight section
Bunch Compressor Beam Line Optics
Feasibility of Reusing PEP-II Hardware for MEIC Electron Ring
Ion Collider Ring Using Superferric Magnets
Fanglei Lin, Yuhong Zhang JLEIC R&D Meeting, March 10, 2016
Update on JLEIC Electron Ring Design
Fanglei Lin MEIC R&D Meeting, JLab, July 16, 2015
Possibility of MEIC Arc Cell Using PEP-II Dipole
Fanglei Lin JLEIC R&D Meeting, August 4, 2016
Presentation transcript:

CW Linac: Optics with Quads or Doublets. N. Perunov and N.Solyak Nov.6, 2009

Focusing in current v.1 ICD-2 lattice. Period = 3808 mm Q: L/L_eff =520/200 mm Aperture = 44 mm B’ = 12 T/m TSR: SSR0: SSR1: Sol+drift+Cav+drift =560mm = Aperture = 30 mm Drift+Sol+drift+Cav=750mm = Aperture = 30 mm SSR2: drift+Sol+drift+Cav+drift+Cav+drift= =1600 mm Aperture = 30 mm Solenoid Quads

CW Linac (v.1 Oct.01, 2009) Focusing lengths of quads and cavities.

Quad focusing - v1. SSR2 section: FRDR TRACE-3D TRACK I = 10 mA

SSR2 : Doublet focusing (quad separation = 6 cm) Phase advance per focusing period. I = 0 mA 3 mm TRACE-3D I = 0 mA TRACK 3 mm Foc. period = 166 cm B’=16.8 T/m (phase advance = 85 deg)

3 mm TRACK 3 mm TRACE-3DI = 0 mA SSR2 : Doublet focusing (quad separation = 0 cm) Foc. period = 160 cm B’=19.8 T/m (phase adv. = 85 deg)

3 mm TRACE-3DI = 0 mA. 3 mm TRACK I = 0 mA. Eff. quad length = 10 cm Length of quad = 16 cm. Focusing period = 74 cm B’=23 T/m for transv. phase advance 85 deg. 90 Phase advance long. tr. SSR1: Doublet focusing - v1. (1CM=9*(FDR)+drift).

3 mm TRACE-3D I = 0 mA 3 mm TRACKI = 0 mA Quad length = 18 cm Quad Leff = 12 cm. Foc period = 78 cm. B’=18 T/m (phase advance 85 deg) Phase advance 90 tr. long. SSR1: Doublet focusing – v2. (1CM=9*(FDR)+FD+drift).

SSR0: Doublet focusing (1CM=(FDR)*16+drift) Version 1 #SSR0 1 period begin 1 drift quad drift quad drift cav #SSR0 1 period end Effective quad length = 10 cm. Length of quad = 16 cm. Length of focusing period = 65.4 cm. B’=13.5 T/m for transverse phase advance 85 deg. Version 2 #SSR0 1 period begin 1 drift quad drift quad drift cav #SSR0 1 period end Effective quad length = 8 cm. Length of quad = 14 cm. Length of focusing period = 61.4 cm. B’=17.5 T/m for transverse phase advance 85 deg. 100 Phase advance tr. long. 100 Phase advance tr. long.

SSR0: Doublet focusing v3. (1CM=16 * (FDR) +drift) Version 3 #SSR0 1 period begin 1 drift quad drift quad drift cav #SSR0 1 period end Effective quad length = 8 cm. Length of quad = 14 cm. Length of focusing period = 55.4 cm. B’=21.4 T/m for transverse phase advance 85 deg. 90 Phase advance tr. long. 3 mm TRACK I = 0 mA 10 deg. 3 mm I = 0 mA 12 deg. TRACE-3D

Next steps forward FODO Define more accurate quad parameters with experts (V.Kashikhin) Review configuration of SSR1 cryomodule to reduce bump in beam size due to large extra drift between CM’s Use doublet focusing instead of Quad focusing in TSR section Match SSR0+SSR1+SSR2+TSR Use 9-cell beta=0.81 cavities (new field map) in S-ILC. CM configuration = R+(FD) R 3 +(FD)+ R 3 +(FD)+R 2 (Francois) S-ILC cryomodule is not ILC type with shorter cavities, short doublets and shorter drifts. Design will be done by India (see presentation and Arun talk)