Vertical Dogleg Options for the Ion Collider Ring

Slides:



Advertisements
Similar presentations
Ion Polarization Control in MEIC Rings Using Small Magnetic Fields Integrals. PSTP 13 V.S. Morozov et al., Ion Polarization Control in MEIC Rings Using.
Advertisements

Operated by JSA for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility EIC Collaboration Meeting, Hampton University, May 19-23,
CASA Collider Design Review Retreat HERA The Only Lepton-Hadron Collider Ever Been Built Worldwide Yuhong Zhang February 24, 2010.
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,
Present MEIC IR Design Status Vasiliy Morozov, Yaroslav Derbenev MEIC Detector and IR Design Mini-Workshop, October 31, 2011.
Hybrid Fast-Ramping Synchrotron to 750 GeV/c J. Scott Berg Brookhaven National Laboratory MAP Collaboration Meeting March 5, 2012.
Optics considerations for PS2 October 4 th, 2007 CARE-HHH-APD BEAM’07 W. Bartmann, M. Benedikt, C. Carli, B. Goddard, S. Hancock, J.M. Jowett, A. Koschik,
Optics solutions for the PS2 ring February 11 th, 2008 LIS Section Meeting Y. Papaphilippou.
JLEIC Electron Collider Ring Design and Polarization
Dispersion correction in the bypass dogleg
J-PARC main ring lattice An overview
Ion Collider Ring: Design and Polarization
Acknowledgements and credits to: W. Herr, B. Holzer, A. Streun, A
Large Booster and Collider Ring
Non-linear Beam Dynamics Studies for JLEIC Electron Collider Ring
CEPC pretzel scheme study
Alternate Lattice for LCLS-II LTU Y
First Look at Nonlinear Dynamics in the Electron Collider Ring
Electron collider ring Chromaticity Compensation and dynamic aperture
Electron Ring Optics Design
Specifications for the JLEIC IR Magnets
Collider Ring Optics & Related Issues
Optics solutions for the PS2 ring
Negative Momentum Compaction lattice options for PS2
Comparison of NMC rings for PS2
Accelerator and Interaction Region
Towards an NMC Ring: Dispersion suppressor & long straight section
Optics considerations for PS2
Update on Alternative Design of jleic ion injector Complex B
Negative Momentum Compaction lattice options for PS2
Yuri Nosochkov Yunhai Cai, Fanglei Lin, Vasiliy Morozov
Towards an NMC Ring: Dispersion suppressor & long straight section
JLEIC Collider Rings’ Geometry Options
Progress on Non-linear Beam Dynamic Study
Feasibility of Reusing PEP-II Hardware for MEIC Electron Ring
Path Length Chicane Options
Fanglei Lin, Andrew Hutton, Vasiliy S. Morozov, Yuhong Zhang
Update on MEIC Nonlinear Dynamics Work
Racetrack Booster Option & Initial Spin Tracking Results
Transfer Line for EIC.
Rough designs for The LEB and HEB for pCDR-100
The MEIC electron ring as the large ion booster
Ion Collider Ring Using Superferric Magnets
Fanglei Lin, Yuhong Zhang JLEIC R&D Meeting, March 10, 2016
Alternative Ion Injector Design
Fanglei Lin, Yuri Nosochkov Vasiliy Morozov, Yuhong Zhang, Guohui Wei
Update on JLEIC Electron Ring Design
Conventional Synchronization Schemes
Fanglei Lin MEIC R&D Meeting, JLab, July 16, 2015
Compensation of Detector Solenoids
G.H. Wei, V.S. Morozov, Fanglei Lin Y. Nosochkov (SLAC), M-H. Wang
JLEIC Collider Rings’ Geometry Options (II)
Progress Update on the Electron Polarization Study in the JLEIC
Integration of Detector Solenoid into the JLEIC ion collider ring
First results of proton spin tracking in a figure-8 ring
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
Arc FODO Cell Inventory
Update on MEIC Nonlinear Dynamics Work
Fanglei Lin JLEIC R&D Meeting, August 4, 2016
MEIC R&D Meeting, JLab, August 20, 2014
Summary of JLEIC Electron Ring Nonlinear Dynamics Studies
Update on MEIC Nonlinear Dynamics Work
DYNAMIC APERTURE OF JLEIC ELECTRON COLLIDER
Update on the High Energy Booster Design
A TME-like Lattice for DA Studies
Illustrations of Beam Synchronization Issue
MOPRB098 An Increased Extraction Energy Booster Complex For The Jefferson Lab Electron Ion Collider* Thomas Jefferson National Accelerator Facility Newport.
Presentation transcript:

Vertical Dogleg Options for the Ion Collider Ring V.S. Morozov, Y. Nosochkov JLEIC Weekly R&D Meeting September 8, 2016 F. Lin

General Considerations Doglegs for vertically stacking the electron and ion collider beam lines in the arc sections Constraints Cannot interleave net rotations about different axis to avoid breaking the figure-8 spin symmetry Have to manage horizontal and vertical dispersions Minimize total length and magnet strengths for a given size of the vertical step (in the following assumed to be 1 m, need engineering feedback) Dogleg options Single step, e.g. bend down + ~2 vertical betatron phase advance + bend up Two step (á la CEBAF), e.g. down/up dipole step +  vertical betatron phase advance + down/up dipole step Combined vertical and horizontal bends, e.g. down/up dipole step + horizontally bending section with  vertical betatron phase advance + down/up dipole step

Dogleg Option I: Single Step Achromatic Can provide relatively large vertical step size Size dominated by the space necessary to accumulate the 2 vertical betatron phase advance  to reduce it, use 1.6 m long (2 x regular) quadrupoles with maximum gradient of 52.3 T/m at 100 GeV/c Yuri: it may be worth inserting another quadrupole

Dogleg Option II: Two Step Achromatic More efficient for a relatively small vertical step size Lengths of the dipole pairs contribute significantly to the total size Use 1.6 m long (2 x regular) quads with maximum gradient of 50.0 T/m at 100 GeV/c

Dogleg Option IIa: Two Step Yuri’s suggestion: use standard 90 cells with periodic beta functions with the same polarity dipoles placed 2 cells apart (i.e. 180 deg apart) Bigger step with regular optics but longer

Dogleg Option III: Combined Achromatic for vertical dispersion, matched directly to a regular arc FODO cell and suppresses horizontal dispersion (-) Involves a larger number of quadrupole families Provides horizontal bend of one regular arc FODO cell More efficient for a relatively small vertical step size Lengths of the dipole pairs contribute significantly to the total size (+) May be a better geometric match to the electron beam line  smaller tunnel Use 1.6 m long (2 x regular) quads with maximum gradient of 46.1 T/m at 100 GeV/c

Conclusions All three dogleg options have comparable lengths for 1 m vertical step size Need engineering feedback Smaller step size would favor options II and III while larger step size would favor option I Despite its relative complexity, option III has an important potential benefit of providing a better geometric match to the electron beam line Need to wait for the next-iteration electron ring layout to make a selection