Status of RHIC Polarization Studies. Summary of Polarization Studies during Run09 Tune scans: – Nearby 0.7 – Near integer tune Polarization ramp measurement.

Slides:



Advertisements
Similar presentations
Note: most of the slides shown here are picked from CERN accelerator workshops. Please refer to those workshop for further understanding of the accelerator.
Advertisements

SESAME – TAC 2012: M. Attal Maher Attal SESAME Booster Characterization.
RHIC Status Haixin Huang Time Meeting 02/1/2011. Jan. 26 Ring access for six hours to fix jet and many other jobs. Difficulty to provide 28X28 store overnight.
Accelerating Polarized Protons Mei Bai Collider Accelerator Department Brookhaven National Laboratory PHNIX Focus, Feb. 24,
Nov. 17, 2005Fermi Lab AP Seminar AC Dipole Based Diagnostics Mei Bai, C-A Department.
AC dipole for LHC Mei Bai Collider Accelerator Department Brookhaven National Laboratory.
AGS pp Status Feb. 20, 2015 RSC Meeting Haixin Huang.
AGS Polarized Proton Development toward Run-9 Oct. 3, 2008 Haixin Huang.
Beam-beam Observations in RHIC Y. Luo, W. Fischer Brookhaven National Laboratory, USA ICFA Mini-workshop on Beam-Beam Effects in Hadron Colliders, March.
Overview Run-6 - RHIC Vadim Ptitsyn C-AD, BNL. V.Ptitsyn RHIC Spin Workshop 2006 RHIC Run-6 Timeline  1 Feb – Start of the Run-6. Start of the cooldown.
RHIC Accelerator Capability: Present and Future Mei Bai Collider Accelerator Dept. BNL.
Thomas Roser Snowmass 2001 June 30 - July 21, 2001 Polarized Proton Acceleration and Collisions Spin dynamics and Siberian Snakes Polarized proton acceleration.
Injector PP Setup Plan and Status November 18, 2008 Haixin Huang.
October 4-5, Electron Lens Beam Physics Overview Yun Luo for RHIC e-lens team October 4-5, 2010 Electron Lens.
May 17, 2005Wednesday Experiment Meeting BNL, Upton Acceleration beyond 100 GeV  Goal To evaluate the spin dynamics beyond 100 GeV  What’s the impact.
Preparation for RHIC PP Run in 2011 Wednesday 20, 2010 RHIC Machine Planning Meeting Haixin Huang RUN website: RUN.
Overview of RHIC Injector Oct. 5, 2015 Haixin Huang MEIC 2015.
Plans for Polarized Beams at VEPP-2000 and U-70 Yu.Shatunov BINP, Novosibirsk P S IN 2006.
RHIC Status: Startup Run 12 V. Schoefer RHIC Spin Collaboration Meeting 1/13/12.
Spin Injection June 5, 2015 APEX Meeting H. Huang, P. Oddo, V. Ptitsyn.
RHIC pp 500 GeV development M. Bai C-A Department.
APEX Report: February 26-27, 2008 Fulvia Pilat Time Meeting, March 4, 2008.
RHIC Run11 Summary May 6, 2011 RSC Meeting Haixin Huang Luminosity Availability Polarization RHIC setup issues.
Feb. 23, 2005Wednesday Experiment Meeting BNL, Upton Status on AGS cold snake  Cold mass is now in the cryostat. It is in the phase of wiring, and because.
J-PARC Spin Physics Workshop1 Polarized Proton Acceleration in J-PARC M. Bai Brookhaven National Laboratory.
Simulation of Spin Interference and Echo Effect Abstract Successively jumping across a depolarization resonance twice produces interesting spin dynamics.
POLARIZATION MEASUREMENTS AND ABSOLUTE POLARIZATION VALUES EVOLUTION DURING PROTON BEAM ACCELERATION IN THE RHIC ACCELERATOR COMPLEX A.Zelenski, T.Roser,
RHIC Store Energy Scan Mei Bai Collider Accelerator Dept. Brookhaven National Laboratory.
AGS Run-9 Preparations, Status and Plans Dec. 16, 2008 Haixin Huang.
Thomas Roser SPIN 2008 October 10, 2008 The Future of High Energy Polarized Proton Beams Spin dynamics and depolarizing resonances Early multi-GeV polarized.
09-21 Study of bunch length limits Goals: To identify and observe effects which put limits on the minimum bunch length in RHIC. Try to distiguish the limitation.
Beam-beam compensation at RHIC LARP Proposal Tanaji Sen, Wolfram Fischer Thanks to Jean-Pierre Koutchouk, Frank Zimmermann.
Orbit related issues of the spin tune control at RHIC V.Ptitsyn, M.Bai, W.MacKay, T.Roser.
First Demonstration of Optics Measurement and Correction during Acceleration Chuyu Liu Collider Accelerator Department, BNL.
Accelerating Polarized Protons to High Energy Mei Bai Collider Accelerator Department Brookhaven National Laboratory.
Thomas Roser Derbenev Symposium August 2-3, 2010 Polarized Beam Acceleration In their seminal paper “Radiative Polarization: Obtaining, Control, Using”
Polarized Proton at RHIC: Status and Future Plan Mei Bai Collider Accelerator Dept. BNL A Special Beam Physics Symposium in Honor of Yaroslav Derbenev's.
RHIC Status April 8, 2011 RSC Meeting Haixin Huang.
Run 10 Start-up Status
Haixin Huang AGS Cold Snake: Status and Plans.
APEX Studies: Accelerating w. Near 3 rd Order Resonance Vincent, Al, Michiko, Steve, Don, Yun, Guillaume, Mei, Todd, Wolfram, Greg, …
RHIC Status Haixin Huang RSC Meeting 02/18/2011. l Fixed the blue dump kicker noise problem last Friday. l Declared physics last Friday. l Smooth run.
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,
Plan for 500 GeV Development Vadim, Mei. Goals 1.Explore polarization transmission to the 500 Gev CM energy. 2. Inspect the luminosity aspects (with 2.
AGS FY11 Summary RHIC Spin Collaboration Meeting 5/6/11.
APEX Status and Plan Phil’s Meeting, March 20, 2012 M. Bai.
RHIC Status Haixin Huang Time Meeting 01/25/2011.
Polarized Proton Acceleration in the AGS with Two Helical Partial Snakes October 2, 2006 SPIN 2006 H. Huang, L.A. Ahrens, M. Bai, A. Bravar, K. Brown,
Deuteron Polarization in MEIC
Acceleration of Polarized Protons and Deuterons at HESR/FAIR
Field quality to achieve the required lifetime goals (single beam)
Preservation and Control of Ion Polarization in MEIC
Electron Polarization In MEIC
Possibility for polarized beam at J-PARC Summary of Satellite Workshop on Polarized Proton Beam at J-PARC Satellite Workshop Program: Overview of the status.
The new 7BA design of BAPS
I Alexander Nass for the JEDI collaboration
PEPX-type BAPS Lattice Design and Beam Dynamics Optimization
JLEIC Collaboration meeting Spring 2016 Ion Polarization with Figure-8
Spin Transparency Study and Test
RHIC Spin Flipper M. Bai, T. Roser Collider Accelerator Department
Update on MEIC Ion Polarization Work
JLEIC Weekly R&D Meeting
Summary of Working Group 1
Yu.N. Filatov, A.M. Kondratenko, M.A. Kondratenko
Progress Update on the Electron Polarization Study in the JLEIC
First results of proton spin tracking in a figure-8 ring
Status of Proton & Deuteron Spin Tracking in Racetrack Booster
Current Status of Ion Polarization Studies
Summary and Plan for Electron Polarization Study in the JLEIC
Status of RCS eRHIC Injector Design
Presentation transcript:

Status of RHIC Polarization Studies

Summary of Polarization Studies during Run09 Tune scans: – Nearby 0.7 – Near integer tune Polarization ramp measurement – 28/56 bunches – At both working points Spin tune as function of horizontal orbital angle at snake – 100 GeV and 250 GeV

Polarization Status: 250 GeV polarization were lost beyond 100 GeV to 250 GeV Average polarization transmission efficiency: ~80% Best polarization achieved w.o. rotator: ~54%

Polarization ramp measurement: nearInt polarization were lost beyond 100 GeV to 250 GeV Average polarization transmission efficiency: ~80% Best polarization achieved w.o. rotator: ~54%

Tune Scan of 250GeV: gg260, gg381, gg422 7/10 resonance 11/16 resonance 3/4 resonance Working pt for 250 GeV run

Investigating polarization at near Integer Orbit deteriorated rms ~0.5mm Orbit rms ~ 0.2mm Zero the snake orb angle

What did we learn from near integer tune study Polarization transmission efficiency reached plateau for Qy = and above, as expected However, it didn’t exceed what was achieved at working point close to 2/3 resonance, and the best achieved polarization is only 50%, also below what we had with the other working point, not as expected. Possible speculations – Stronger intrinsic resonance strength – Stronger imperfection resonance due to closed orbit distortion No information on closed orbit at defocusing quads where there are no bpms – Need detailed studies to see the above effects More realistic model of RHIC for simulation Data of measured spin direction w.o. rotator to check whether stable spin direction is vertical

Status of spin tracking using zgoubi A matured code developed at F. Moet and S. Valero.Calculate beam dynamics as well as spin dynamics by integrating through magnetic field. The original version has no snakes. Provide cross-check with spin tracking using spink Currently, – Testing the spin tracking of zgoubi Compared the net spin rotation through a RHIC dipole by zgoubi – Agreed up to 10^-4 degrees for a hard edge magnet and 10^-3 degrees with fridge field included Check the main depolarization resonances at RHIC with no snake Repeat with snakes. Currently, snakes are represented as two perfect 180 degree spin rotators which are perfect drift for orbital motion. Add ac dipole – Bench mark zgoubi with experimental data Polarization tune scan data in RUN09 Spin flipper data in RUN09 – Detailed spin tracking with closed orbit errors

Spin Flipper Status New design: localize the ac ipole driven oscillation within spin flipper Add three new ac dipoles. Increase the DC dipole current to 1500 Amps Rotating field strength: Ac dipole DC dipole

Spin Flipper Status Plan for RUN03 is to test the closure ac dipole bump Adding the ac dipole in the middle of the the spin flipper Expect magnet coil early Nov. Expect magnet stand mid of Oct. Installation will begin once it is available. Vacuum work including installation of the ceramic pipe first week of Nov. Magnet will be installed during maintainence Measure the residual coherent oscillation beyond spin flipper

How to achieve >50% polarization at 250 GeV? Polarization transmission efficiency –Explore the possibility of accelerating polarized protons at working point between –250 GeV tune scan data indicates a polarization transmission efficiency of 90% and more can be achieved –Assuming polarization at RHIC injection reaches >60%, the polarization at 250 GeV can reach > 50% Polarization lifetime: detailed data analysis -What’s impact of Blue PHENIX rotator setting on spin tune? -Did the local orbit at rotators matter? Should demonstrate the correlation from the data Optimize the snake setting (current and orbital angle) at store based on the spin tune measurement Revisit spin tracking -Bench making spin tracking code(s) using experimental data

Spin tune as function of H orbital angle between snakes Measurements were done at 100 GeV as well as 250 GeV These data sets will allow us to distinguish the contribution to the spin tune shift from snake imperfection and from horizontal angle between snakes

Spin tune as function of H orbital angle between snakes Blue Qy = 0.74

Spin tune as function of H orbital angle between snakes Yellow Qy = 0.744

Polarization Lifetime: 250 GeV Polarization lifetime is very sensitive to the PHENIX rotator setting

Investigating polarization at near Integer Orbit deteriorated rms ~0.5mm Orbit rms ~ 0.2mm Zero the snake orb angle