Alex Bogacz, Geoff Krafft and Timofey Zolkin

Slides:



Advertisements
Similar presentations
MCDW 2008, JLAB, Dec 8-12, Multi-pass Droplet Arc Design Guimei WANG (Muons Inc./ODU) Dejan Trbojevic (BNL) Alex Bogacz (JLAB)
Advertisements

Wilson Lab Tour Guide Orientation 11 December 2006 CLASSE 1 Focusing and Bending Wilson Lab Tour Guide Orientation M. Forster Mike Forster 11 December.
Operated by JSA for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility 1 Lecture 15  Radiation Damping Radiation Damping USPAS,
1 IR with elliptical compensated solenoids in FCC-ee S. Sinyatkin Budker Institute of Nuclear Physics 13 July 2015, CERN.
Operated by JSA for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility EIC Collaboration Meeting, Hampton University, May 19-23,
ELIC Low Beta Optics with Chromatic Corrections Hisham Kamal Sayed 1,2 Alex Bogacz 1 1 Jefferson Lab 2 Old Dominion University.
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.
Operated by JSA for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility 1 Lecture 5  Magnetic Multipoles Magnetic Multipoles,
Operated by JSA for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility Muon Collider Design Workshop, BNL, December 1-3, 2009.
Operated by the Southeastern Universities Research Association for the U.S. Depart. Of Energy Thomas Jefferson National Accelerator Facility Alex Bogacz,
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.
Operated by the Southeastern Universities Research Association for the U.S. Depart. Of Energy Thomas Jefferson National Accelerator Facility Alex Bogacz,
Operated by JSA for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility Alex Bogacz Status and Plans for Linac and RLAs.
Operated by JSA for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility Alex Bogacz 1 Status of Baseline Linac and RLAs Design.
Operated by JSA for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility Alex Bogacz 1 Muon Acceleration – RLA, FFAG and Fast Ramping.
Lecture 5 - E. Wilson - 6/29/ Slide 1 Lecture 5 ACCELERATOR PHYSICS MT 2014 E. J. N. Wilson.
Operated by JSA for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility Alex Bogacz IDS- NF Acceleration Meeting, Jefferson Lab,
Operated by JSA for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility Alex Bogacz 1 Recirculating Linac Acceleration  End-to-end.
Operated by JSA for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility Alex Bogacz NuFact’08, Valencia, Spain, July 4, 2008 Alex.
Progress on the Linac and RLAs
JLEIC simulations status April 3rd, 2017
Parametric Resonance Ionization Cooling of Muons
PERLE - Current Accelerator Design
Large Booster and Collider Ring
Progress on the Linac and RLAs
‘Multi-pass-Droplet’ Experiment
First Look at Nonlinear Dynamics in the Electron Collider Ring
Status of Linac and RLAs – Simulations
Muon RLA - Design Status and Simulations
Muon RLA - Design Status and New Options
Linac and RLAs – Overview of NF-IDS
Electron Ring Optics Design
LHC (SSC) Byung Yunn CASA.
Progress on the Linac and RLAs
Collider Ring Optics & Related Issues
Optics ‘Scrapbook’ for ERL Test Facility
RLA WITH NON-SCALING FFAG ARCS
Optics and Layout of Alex Bogacz Workshop, Orsay, Feb. 23, 2017.
Accelerator and Interaction Region
Low Emittance Lattices
Betatron Motion with Coupling of Horizontal and Vertical Degrees of Freedom – Part II Alex Bogacz USPAS, Hampton, VA, Jan , 2011.
S.A. Bogacz, G.A. Krafft, S. DeSilva and R. Gamage
Radiation Damping S.A. Bogacz, G.A. Krafft, S. DeSilva and R. Gamage
Synchrotron Motion S.A. Bogacz, G.A. Krafft, S. DeSilva and R. Gamage
Muon RLA - Design Status and New Options
Alex Bogacz, Geoff Krafft and Timofey Zolkin
– Overview Alex Bogacz JLAB, Aug. 14, 2017.
Alex Bogacz, Geoff Krafft and Timofey Zolkin
Lecture 5 ACCELERATOR PHYSICS MT 2009 E. J. N. Wilson.
Muon RLA - Design Status and Simulations
Vertical Dogleg Options for the Ion Collider Ring
Progress on Non-linear Beam Dynamic Study
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
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
JLEIC Electron Ring Nonlinear Dynamics Work Plan
Upgrade on Compensation of Detector Solenoid effects
Fanglei Lin JLEIC R&D Meeting, August 4, 2016
Booster to Ion Ring Transfer Line
Large Ion Booster Re-design Update
PERLE - Current Accelerator Design
Presentation transcript:

Alex Bogacz, Geoff Krafft and Timofey Zolkin Betatron Motion with Coupling of Horizontal and Vertical Degrees of Freedom – Part II Alex Bogacz, Geoff Krafft and Timofey Zolkin USPAS, Fort Collins, CO, June 10-21, 2013

Outline Practical Examples: Spin Rotator for Figure-8 Collider ring Vertex-to-plane adapter for electron cooling (Fermilab) Ionization cooling channel for Neutrino Factory and Muon Collider Generalized vertex-to-plane transformer insert V. Lebedev, A. Bogacz, ‘Betatron Motion with Coupling of Horizontal and Vertical Degrees of Freedom’, 2000, http://dx.doi.org/10.1088/1748-0221/5/10/P10010 USPAS, Fort Collins, CO, June 10-21, 2013

Axisymmetric rotational distribution - Twiss functions USPAS, Fort Collins, CO, June 10-21, 2013

Axisymmetric rotational distribution - Twiss functions USPAS, Fort Collins, CO, June 10-21, 2013

Axisymmetric rotational distribution - Twiss functions USPAS, Fort Collins, CO, June 10-21, 2013

Axisymmetric rotational distribution - Twiss functions USPAS, Fort Collins, CO, June 10-21, 2013

Spin rotators for Figure-8 Collider Ring total ring circumference ~1000 m 60 deg. crossing USPAS, Fort Collins, CO, June 10-21, 2013

Spin Rotator - Ingredients… 320 230 15 0.15 -0.15 BETA_X&Y[m] DISP_X&Y[m] BETA_X BETA_Y DISP_X DISP_Y Arc end 4.4 0 8.8 0 Spin rotator ~ 46 m BL = 11.9 Tesla m BL = 28.7 Tesla m USPAS, Fort Collins, CO, June 10-21, 2013

Locally decoupled solenoid pair 17.9032 15 5 BETA_X&Y[m] BETA_1X BETA_2Y BETA_1Y BETA_2X BL = 28.7 Tesla m solenoid 4.16 m solenoid 4.16 m decoupling quad insert M = C - C Hisham Sayed, PhD Thesis ODU, 2011 USPAS, Fort Collins, CO, June 10-21, 2013

Locally decoupled solenoid pair 17.9032 15 1 -1 BETA_X&Y[m] DISP_X&Y[m] BETA_X BETA_Y DISP_X DISP_Y BL = 28.7 Tesla m solenoid 4.16 m solenoid 4.16 m decoupling quad insert M = C - C Hisham Sayed, PhD Thesis ODU, 2011 USPAS, Fort Collins, CO, June 10-21, 2013

Universal Spin Rotator - Optics 5 GeV 374 288 30 1 -1 BETA_X&Y[m] DISP_X&Y[m] BETA_X BETA_Y DISP_X DISP_Y 4.4 0 8.8 0 Spin rotator ~ 46 m BL = 11.9 Tesla m BL = 28.7 Tesla m USPAS, Fort Collins, CO, June 10-21, 2013

Ionization Cooling in an Axially Symmetric Channel USPAS, Fort Collins, CO, June 10-21, 2013

Ionization Cooling in an Axially Symmetric Channel USPAS, Fort Collins, CO, June 10-21, 2013

Ionization Cooling in an Axially Symmetric Channel USPAS, Fort Collins, CO, June 10-21, 2013

Hamiltonian formulation - equations of motion USPAS, Fort Collins, CO, June 10-21, 2013

Ionization Cooling in an Axially Symmetric Channel USPAS, Fort Collins, CO, June 10-21, 2013

Ionization Cooling in an Axially Symmetric Channel USPAS, Fort Collins, CO, June 10-21, 2013

Ionization Cooling in an Axially Symmetric Channel USPAS, Fort Collins, CO, June 10-21, 2013

Ionization Cooling in an Axially Symmetric Channel USPAS, Fort Collins, CO, June 10-21, 2013

Ionization Cooling in an Axially Symmetric Channel USPAS, Fort Collins, CO, June 10-21, 2013

Ionization Cooling in an Axially Symmetric Channel USPAS, Fort Collins, CO, June 10-21, 2013

Ionization Cooling in an Axially Symmetric Channel USPAS, Fort Collins, CO, June 10-21, 2013

Beta functions in axially symmetric FOFO cell USPAS, Fort Collins, CO, June 10-21, 2013

Periodic Cell - Optics ‘inward half-cell’ ‘outward half-cell’ betatron phase adv/cell (h/v) = p/2p USPAS, Fort Collins, CO, June 10-21, 2013

Periodic Cell – Magnets ‘inward half-cell’ ‘outward half-cell’ betatron phase adv/cell (h/v) = p/2p solenoids: L[cm] B[kG] 22 105 22 105 quadrupoles: L[cm] G[kG/cm] 8 1.79754 8 -0.3325 dipoles: $L=20; => 20 cm $B= 25; => 25 kGauss $Ang=$L*$B/$Hr; => 0.4996 rad $ang=$Ang*180/$PI; => 28.628 deg USPAS, Fort Collins, CO, June 10-21, 2013

‘Snake’ cooling channel – Dispersion suppression entrance cell periodic cells exit cell USPAS, Fort Collins, CO, June 10-21, 2013

Muon Cooling Channel - Optics beam extension disp. anti-suppr. disp. suppr. beam extension RF cavity skew quad n periodic PIC/REMEX cells (n=2) USPAS, Fort Collins, CO, June 10-21, 2013

Vertex-to-plane transformer insert USPAS, Fort Collins, CO, June 10-21, 2013

Vertex-to-plane transformer insert USPAS, Fort Collins, CO, June 10-21, 2013

Vertex-to-plane transformer insert USPAS, Fort Collins, CO, June 10-21, 2013

Vertex-to-plane transformer insert 2.62647 1 5 BETA_X&Y[m] BETA_1X BETA_2Y BETA_1Y BETA_2X -1 Betatron size X&Y[cm] AlphaXY[-1, +1] Ax Ay AlphaXY 0.5 PHASE/(2*PI) Q_1 Q_2 Teta1 Teta2 USPAS, Fort Collins, CO, June 10-21, 2013

Summary USPAS, Fort Collins, CO, June 10-21, 2013