JLEIC Weekly R&D Meeting

Slides:



Advertisements
Similar presentations
Flipping proton and deuteron spins in storage rings L.I. Malysheva.
Advertisements

Searching for CesrTA guide field nonlinearities in beam position spectra Laurel Hales Mike Billing Mark Palmer.
Accelerating Polarized Protons Mei Bai Collider Accelerator Department Brookhaven National Laboratory PHNIX Focus, Feb. 24,
Simulation of direct space charge in Booster by using MAD program Y.Alexahin, N.Kazarinov.
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.
Development of Simulation Environment UAL for Spin Studies in EDM Fanglei Lin December
Multiple spin resonance crossing in accelerators. A.M. Kondratenko (1), M.A. Kondratenko (1) and Yu. N. Filatov (2) (1) GOO “Zaryad”, Novosibirsk (2) JINR,
October 4-5, Electron Lens Beam Physics Overview Yun Luo for RHIC e-lens team October 4-5, 2010 Electron Lens.
Simulation of direct space charge in Booster by using MAD program Y.Alexahin, A.Drozhdin, N.Kazarinov.
Control of Beam Polarization at the NICA Collider A.M. Kondratenko 2, A.D. Kovalenko 1, M.A. Kondratenko 2, Yu.N. Filatov 1,3 and V.A. Mikhaylov 1 1 Join.
E Levichev -- Dynamic Aperture of the SRFF Storage Ring Frontiers of Short Bunches in Storage Rings INFN-LNF, Frascati, 7-8 Nov 2005 DYNAMIC APERTURE OF.
Polarization in ELIC Yaroslav Derbenev Center for Advanced Study of Accelerators Jefferson Laboratory EIC Collaboiration Meeting, January 10-12, 2010 Stony.
J-PARC Spin Physics Workshop1 Polarized Proton Acceleration in J-PARC M. Bai Brookhaven National Laboratory.
RHIC Store Energy Scan Mei Bai Collider Accelerator Dept. Brookhaven National Laboratory.
Thomas Roser SPIN 2008 October 10, 2008 The Future of High Energy Polarized Proton Beams Spin dynamics and depolarizing resonances Early multi-GeV polarized.
By Verena Kain CERN BE-OP. In the next three lectures we will have a look at the different components of a synchrotron. Today: Controlling particle trajectories.
Thomas Roser Derbenev Symposium August 2-3, 2010 Polarized Beam Acceleration In their seminal paper “Radiative Polarization: Obtaining, Control, Using”
1 Polarized Proton Beam Acceleration at Nuclotron with the use of the Solenoid Siberian Snake Yu.N. Filatov 1,3, A.D. Kovalenko 1, A.V. Butenko 1, A.M.
Present MEIC IR Design Status Vasiliy Morozov, Yaroslav Derbenev MEIC Detector and IR Design Mini-Workshop, October 31, 2011.
Compensation of Detector Solenoid G.H. Wei, V.S. Morozov, Fanglei Lin JLEIC Collaboration Meeting Spring, 2016.
Lecture 4 Longitudinal Dynamics I Professor Emmanuel Tsesmelis Directorate Office, CERN Department of Physics, University of Oxford ACAS School for Accelerator.
1 Error study of non-scaling FFAG 10 to 20 GeV muon ring Shinji Machida CCLRC/RAL/ASTeC 26 July, ffag/machida_ ppt.
Thomas Roser SPIN 2006 October 3, 2006 A Study of Polarized Proton Acceleration in J-PARC A.U.Luccio, M.Bai, T.Roser Brookhaven National Laboratory, Upton,
Status of RHIC Polarization Studies. Summary of Polarization Studies during Run09 Tune scans: – Nearby 0.7 – Near integer tune Polarization ramp measurement.
Polarization of CEPC M. Bai Collider Accelerator Department Brookhaven National Laboratory, Upton, NY Dec , 2013 International workshop on.
JLEIC simulations status April 3rd, 2017
Ion Collider Ring: Design and Polarization
P. Chevtsov for the ELIC Design Team
Deuteron Polarization in MEIC
Large Booster and Collider Ring
Non-linear Beam Dynamics Studies for JLEIC Electron Collider Ring
Acceleration of Polarized Protons and Deuterons at HESR/FAIR
Preservation and Control of Ion Polarization in MEIC
Electron Polarization In MEIC
Polarized Ion Beams with JLEIC
Review of Accelerator Physics Concepts
ICFA Mini-Workshop, IHEP, 2017
JLEIC Ion and Electron Polarization
JLEIC Collaboration meeting Spring 2016 Ion Polarization with Figure-8
Spin Transparency Study and Test
Ion Collider Ring Chromatic Compensation and Dynamic Aperture
RHIC Spin Flipper M. Bai, T. Roser Collider Accelerator Department
Yuri Nosochkov Yunhai Cai, Fanglei Lin, Vasiliy Morozov
Vertical Dogleg Options for the Ion Collider Ring
Racetrack Booster Option & Initial Spin Tracking Results
Update on MEIC Ion Polarization Work
Update on MEIC Ion Polarization Work
Update on MEIC Ion Polarization Work
Update on MEIC Nonlinear Dynamics Work
Current Status for Ion Polarization Studies
Yu.N. Filatov, A.M. Kondratenko, M.A. Kondratenko
M.A. Kondratenko, V.S. Morozov, Y. Zhang
Fanglei Lin, Yuhong Zhang JLEIC R&D Meeting, March 10, 2016
Alejandro Castilla CASA/CAS-ODU
JLEIC Weekly R&D Meeting
Compensation of Detector Solenoids
G.H. Wei, V.S. Morozov, Fanglei Lin Y. Nosochkov (SLAC), M-H. Wang
Update on MEIC Nonlinear Dynamics Work
JLEIC Collider Rings’ Geometry Options (II)
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
First results of proton spin tracking in a figure-8 ring
Upgrade on Compensation of Detector Solenoid effects
Status of Proton & Deuteron Spin Tracking in Racetrack Booster
Fanglei Lin JLEIC R&D Meeting, August 4, 2016
Current Status of Ion Polarization Studies
Summary and Plan for Electron Polarization Study in the JLEIC
DYNAMIC APERTURE OF JLEIC ELECTRON COLLIDER
Report on Electron Polarization Study
Presentation transcript:

JLEIC Weekly R&D Meeting Spin-Tracking the JLEIC Ion Collider Ring: Polarization Control and Spin Flip A.M. Kondratenko, M.A. Kondratenko, and Yu.N. Filatov presented by V.S. Morozov JLEIC Weekly R&D Meeting June 23, 2016 F. Lin

Outline Ideal figure-8 collider ring 3D spin rotator Reference particle Particle with non-zero betatron amplitudes 3D spin rotator Ideal collider ring with spin motion stabilized by a 3D spin rotator Effect of lattice imperfections Closed orbit distortion Coherent part of the zero-integer spin resonance strength Spin control with a single 3D spin rotator Spin control with compensation of the coherent part by a 2nd rotator Spin flip Summary and conclusions

Ideal Figure-8 Collider Lattice A sanity check 60 GeV/c reference proton with initially vertical (Sy) spin 60 GeV/c reference deuteron with initially longitudinal (Sz) spin

Effect of Betatron Oscillations Incoherent component of the zero-integer spin resonance strength 60 GeV/c proton launched with 25/5 m x/y offset at the IP Particles with initially vertical and longitudinal spins The incoherent component is vertical as expected The incoherent part has a strength of 1.810-5 for protons (0.710-9 for deuterons)

3D Spin Rotator Three modules for control of the radial, vertical, and longitudinal spin components Module for control of the radial component (fixed radial orbit bump) Module for control of the vertical component (fixed vertical orbit bump) Module for control of the longitudinal component

3D Rotator Integration Placement of 3D spin rotator elements Location in the lattice

Transverse Proton Polarization Reference proton in an ideal lattice with a 3D spin rotator launched with initially radial and vertical spins; spin tune = 10-2 Proton in an ideal lattice with a 3D spin rotator launched with initially radial and vertical spins with 25/5 m x/y offset at the IP

Longitudinal Deuteron Polarization Reference deuteron in an ideal lattice with a 3D spin rotator launched with initially radial and vertical spins; spin tune = 10-4 Deuteron in an ideal lattice with a 3D spin rotator launched with initially radial and vertical spins with 25/5 m x/y offset at the IP

Lattice Imperfections Transverse quadrupole misalignments Horizontal and vertical closed orbit distortions

New Stable Spin Orientation Longitudinally polarized proton and deuteron launched along closed orbit  Coherent parts of the resonance strengths are 2.5210-3 for protons and 1.14 10-5 for deuterons Proton and deuteron launched along closed orbit with their spins along the stable direction determined by the coherent strength component

Stabilization by 3D Spin Rotators Vertical proton polarization stabilized by a single 3D spin rotator giving a spin tune of 10-2 Oscillations because spin tune of 10-2 is not “much greater” than the coherent resonance strength component of 2.5210-3 After compensation of the coherent component by a 2nd 3D rotator

Spin Flip Adiabaticity criterion: spin reversal time must be much longer than spin precession period  flip >> 1 ms for protons and 0.1 s for deuterons Vertical and longitudinal stable spin direction components as set by the spin rotator vs time Spin tune vs time, changes due to piece-wise linear shape above

Spin Flip Simulation Protons Deuterons at different rates

Summary and Conclusions The ability of a 3D spin rotator to control the ion polarization in the JLEIC energy range has been verified The incoherent part of the resonance strength has been calculated for protons and deuterons setting the limit on the 3D spin rotator strength The coherent part of the resonance strength has been calculated for protons and deuterons using the statistical model Compensation of the coherent part of the resonance strength has been numerically demonstrated A spin flipping system implemented using a 3D rotator for protons and deuterons has been numerically modeled All results obtained so far agree with earlier theoretical and analytical predictions