Update on MEIC Nonlinear Dynamics Work

Slides:



Advertisements
Similar presentations
Full-Acceptance Detector Integration at MEIC Vasiliy Morozov for MEIC Study Group Electron Ion Collider Users Meeting, Stony Brook University June 27,
Advertisements

ELIC Low Beta Optics with Chromatic Corrections Hisham Kamal Sayed 1,2 Alex Bogacz 1 1 Jefferson Lab 2 Old Dominion University.
Dynamic Aperture Study for the Ion Ring Lattice Options Min-Huey Wang, Yuri Nosochkov MEIC Collaboration Meeting Fall 2015 Jefferson Lab, Newport News,
Chromaticity Correction & Dynamic Aperture in MEIC Ion Ring Fanglei Lin MEIC Detector and Interaction Region Designing Mini-Workshop, Oct. 31, 2011.
2 nd Muon Collider Design workshop, JLab, Newport News VA December 8-12, 2008 Update on the Muon Collider lattice design with chromatic correction in IR.
KEKB lattice Taken from LATTICE DESIGN FOR KEKB COLLIDING RINGS By H. Koiso and K. Oide.
Interaction Region Design and Detector Integration V.S. Morozov for EIC Study Group at JLAB 2 nd Mini-Workshop on MEIC Interaction Region Design JLab,
Lattice design for FCC-ee Bastian Haerer (CERN BE-ABP-LAT, Karlsruhe Institute of Technology (KIT)) 1 8 th Gentner Day, 28 October 2015.
Present MEIC IR Design Status Vasiliy Morozov, Yaroslav Derbenev MEIC Detector and IR Design Mini-Workshop, October 31, 2011.
Optics with Large Momentum Acceptance for Higgs Factory Yunhai Cai SLAC National Accelerator Laboratory Future Circular Collider Kick-off Meeting, February.
Optimization of the Collider rings’ optics
Review of new High Energy Rings
Large Booster and Collider Ring
Non-linear Beam Dynamics Studies for JLEIC Electron Collider Ring
First Look at Nonlinear Dynamics in the Electron Collider Ring
Electron collider ring Chromaticity Compensation and dynamic aperture
Nonlinear Dynamics and Error Study of the MEIC Ion Collider Ring
Analysis of Nonlinear Dynamics
XII SuperB Project Workshop LAPP, Annecy, France, March 16-19, 2010
Chromatic Corrections
Collider Ring Optics & Related Issues
Towards an NMC lattice for PS2
Comparison of NMC rings for PS2
SuperB Dynamic Aperture A. Bogomyagkov, E. Levichev, P
Some notes on the SuperB Dynamic Aperture
IR Lattice with Detector Solenoid
Towards an NMC Ring: Dispersion suppressor & long straight section
Yuri Nosochkov Yunhai Cai, Fanglei Lin, Vasiliy Morozov
Multipole Limit Survey of FFQ and Large-beta Dipole
Vertical Dogleg Options for the Ion Collider Ring
JLEIC Collider Rings’ Geometry Options
Progress on Non-linear Beam Dynamic Study
Feasibility of Reusing PEP-II Hardware for MEIC Electron Ring
Fanglei Lin, Andrew Hutton, Vasiliy S. Morozov, Yuhong Zhang
Update on MEIC Nonlinear Dynamics Work
Rough designs for The LEB and HEB for pCDR-100
Update on MEIC Nonlinear Dynamics Work
Update on MEIC Nonlinear Dynamics Work
Yu.N. Filatov, A.M. Kondratenko, M.A. Kondratenko
Ion Collider Ring Using Superferric Magnets
Fanglei Lin, Yuhong Zhang JLEIC R&D Meeting, March 10, 2016
Update on study of chromaticity correction schemes for ion ring
Ion ring lattice with -I sextupole pairs for ir chromaticity correction Y. Nosochkov, M-H. Wang
First Look at Error Sensitivity in MEIC
Fanglei Lin, Yuri Nosochkov Vasiliy Morozov, Yuhong Zhang, Guohui Wei
Update on JLEIC Electron Ring Design
Update on MEIC Nonlinear Dynamics Work
Fanglei Lin MEIC R&D Meeting, JLab, July 16, 2015
G.H. Wei, V.S. Morozov, Fanglei Lin Y. Nosochkov (SLAC), M-H. Wang
Update on MEIC Nonlinear Dynamics Work
Progress Update on the Electron Polarization Study in the JLEIC
Multipole Limit Survey of Large-beta Dipoles
Integration of Detector Solenoid into the JLEIC ion collider ring
G. Wei, V.S. Morozov, Fanglei Lin MEIC R&D Meeting, JLab, Oct 27, 2015
Status of IR / Nonlinear Dynamics Studies
Possibility of MEIC Arc Cell Using PEP-II Dipole
JLEIC Electron Ring Nonlinear Dynamics Work Plan
Upgrade on Compensation of Detector Solenoid effects
Fanglei Lin JLEIC R&D Meeting, August 4, 2016
Summary of JLEIC Electron Ring Nonlinear Dynamics Studies
Chromaticity correction in e-ring with TME cells and –I sextupole pairs in arcs Y. Nosochkov 28 February 2017.
Update on MEIC Nonlinear Dynamics Work
Update on MEIC Nonlinear Dynamics Work
Update on MEIC Nonlinear Dynamics Work
DYNAMIC APERTURE OF JLEIC ELECTRON COLLIDER
A TME-like Lattice for DA Studies
Error Sensitivity in MEIC
Update on DA Studies for a TME-like Lattice
Report on Electron Polarization Study
Update for ion ring lattice chromaticity correction
Presentation transcript:

Update on MEIC Nonlinear Dynamics Work V.S. Morozov Teleconference on Nonlinear Dynamics April 21, 2015 F. Lin

Arc CCB v3 Modified arc FODO lattice matched to regular arc FODO Phase advance between SXT1 adjusted to  Chromatic contribution x = -12.2 and y = -6.3 Sextupole strengths required to compensate 100 units of x/y chromaticity: k2lsxt1/2 = 0.31/-0.66 Contributions to first-order geometric terms due to finite value of x at SXT2 SXT1 SXT2 Re Im h21000 0.04 h30000 -0.013 h10110 -0.18 h10020 1.85 0.09 h10200 2.04 -0.09

Complete Ring Lattice Two identical CCBs integrated: one upstream and one downstream Original (without CCBs) natural x/y chromaticities: -101 / -112 Resulting (with CCBs) natural x/y chromaticities: -121 / -120 The strongest quad in the CCB is ~50% stronger than a regular FODO quad Resulting x/y betatron tunes: 25.598 / 23.733 (can be adjusted) IP

Chromaticity Compensation W functions minimized at the IP and around the ring by tuning the phase advance between the CCBs and the IP (using thin trombones) the sextupole strengths in the CCBs 4 families (two –I pairs and two individual sextupoles) with k2l = -0.10, 0.23, 0.19, -0.37 residual linear x/y chromaticities: -28.5 / -29.1 Residual chromaticities compensated using 2 additional sextupole families 24 sextupoles per family (12 sextupoles of each family in 12 adjacent FODO cells per arc) 90 phase advance between adjacent sextupoles of each family resulting sextupole strengths k2l = 0.25, -0.49 (in the arc with positive dispersion, polarities reversed in the other arc) final ring x/y chromaticities adjusted to +1 / +1 no effect on the W functions outside of the 12 FODO cell blocks before compensation after W function adjustment after residual chromaticity compensation

Higher-Order Chromatic Effects Chromatic tune dependence x,y < 0.02 within |p/p| < ~7p/p Chromatic dependence of *

Conclusions and Outlook Looks okay so far Consistent with Min-Huey’s and Yuri’s earlier result Further work Tracking (have been having some issues with Elegant, will probably use PTC in MAD-X) Optimization 60 FODO cells Uninterleaved sextupoles for residual chromaticity compensation Adjusting the upstream and downstream CCBs independently Upstream CCB only (at the expense of chromatic beam smear at the IP)