Andrew Hutton Concept suggested independently by Haipeng Wang

Slides:



Advertisements
Similar presentations
Chris Tennant Jefferson Laboratory March 15, 2013 “Workshop to Explore Physics Opportunities with Intense, Polarized Electron Beams up to 300 MeV”
Advertisements

Simultaneous Four-Hall Operation for 12 GeV CEBAF Reza Kazimi November 2012.
Possible new EMMA injectors bdm. Motivation ALICE due to shut down soon Alternate EMMA injection (assuming EMMA project continues which it should …) Several.
1 Low-energy RHIC electron Cooler (LEReC) Update November 17, 2014.
Sergey Antipov, University of Chicago Fermilab Mentor: Sergei Nagaitsev Injection to IOTA ring.
Future Very High Luminosity Options for PEP-II John T. Seeman For the PEP-II Team e+e- Factories Workshop October 13-16, 2003.
CSR calculation in ERL merger section Tsukasa Miyajima KEK, High Energy Accelerator Research Organization 8 November, 2010, 13:30 Mini Workshop on CSR.
A fast RF kicker for the MEIC electron cooler Andrew Kimber Amy Sy 31 st March 2015 Thomas Jefferson National Accelerator Facility is managed by Jefferson.
Generation and Characterization of Magnetized Bunched Electron Beam from DC Photogun for MEIC Cooler Laboratory Directed Research and Development (LDRD)
1 Low-energy RHIC electron Cooler (LEReC) cost estimate December 2, 2014.
Thomas Jefferson National Accelerator Facility Page 1 23 rd Annual HUGS Program June 2-20, 2008 CEBAF Overview HUGS08 June 3 CEBAF Overview HUGS08 June.
1 Status of EMMA Shinji Machida CCLRC/RAL/ASTeC 23 April, ffag/machida_ ppt & pdf.
High Current Electron Source for Cooling Jefferson Lab Internal MEIC Accelerator Design Review January 17, 2014 Riad Suleiman.
A 3 Pass, Dog-bone Cooling Channel G H Rees, ASTeC, RAL.
REQUIREMENTS FOR FCC DILUTION KICKERS AND BEAM DUMP LINE GEOMETRY F. Burkart, W. Bartmann, M. Fraser, B. Goddard, T. Kramer FCC dump meeting 18 th June.
Overview of ERL MEIC Cooler Design Studies S.V. Benson, Y. Derbenev, D.R. Douglas, F. Hannon, F. Marhauser, R. A Rimmer, C.D. Tennant, H. Zhang, H. Wang,
Design of an Isochronous FFAG Ring for Acceleration of Muons G.H. Rees RAL, UK.
1 FFAG Role as Muon Accelerators Shinji Machida ASTeC/STFC/RAL 15 November, /machida/doc/othertalks/machida_ pdf/machida/doc/othertalks/machida_ pdf.
Electron Source Configuration Axel Brachmann - SLAC - Jan , KEK GDE meeting International Linear Collider at Stanford Linear Accelerator Center.
CLARA Gun Cavity Optimisation NVEC 05/06/2014 P. Goudket G. Burt, L. Cowie, J. McKenzie, B. Militsyn.
Y. Roblin, D. Douglas, F. Hannon, A. Hofler, G. Krafft, C. Tennant EXPERIMENTAL STUDIES OF OPTICS SCHEMES AT CEBAF FOR SUPPRESSION OF COHERENT SYNCHROTRON.
R.Chehab/ R&D on positron sources for ILC/ Beijing, GENERATION AND TRANSPORT OF A POSITRON BEAM CREATED BY PHOTONS FROM COMPTON PROCESS R.CHEHAB.
Plan for Beam Extraction using strip-line kicker with pulse bump orbit Present extraction kicker system Strip-line kicker system for ILC Beam extraction.
The Introduction to CSNS Accelerators Oct. 5, 2010 Sheng Wang AP group, Accelerator Centre,IHEP, CAS.
Thomas Jefferson National Accelerator Facility Operated by the Southeastern Universities Research Association for the U.S. Department of Energy Harmonic.
MeRHIC Internal Cost Review October, Dmitry Kayran for injector group MeRHIC Internal Cost Review October 7-8, 2009 MeRHIC: Injection System Gun.
Future Circular Collider Study Kickoff Meeting CERN ERL TEST FACILITY STAGES AND OPTICS 12–15 February 2014, University of Geneva Alessandra Valloni.
Development of High Current Bunched Magnetized Electron DC Photogun MEIC Collaboration Meeting Fall 2015 October 5 – 7, 2015 Riad Suleiman and Matt Poelker.
LCLS-II Injector layout design and study Feng Zhou 8/19/2015.
Progress Report on the Ultra-fast Harmonic Kicker Cavity Design and Beam Dynamic Simulation Yulu Huang 1,2 H. Wang 1, R. A. Rimmer 1, S. Wang 1 1.Thomas.
AIP and Large Projects Arne Freyberger OPS 2015 StayTreat.
Preservation of Magnetized Beam Quality in a Non-Isochronous Bend
Beam Commissioning Adam Bartnik.
PIs: Riad Suleiman and Matt Poelker
Options and Recommendations for TL and Dumps
Status and prospects of VEPP-5 Injection Complex
Overview of LERF Status, Plans and Goals
BUNCH LENGTH MEASUREMENT SYSTEM FOR 500 KV PHOTOCATHODE DC GUN AT IHEP
DC Injector and Space Charge Simulation Status
Main magnets for PERLE Test Facility
Joint Accelerator Research JGU & HZB
Junji Urakawa (KEK) for ATF International Collaboration
Magnetized Bunched Electron Beam from DC High Voltage Photogun
The Cornell High Brightness Injector
Capture and Transmission of polarized positrons from a Compton Scheme
Magnetized Electron Beam for Ion Cooling at JLEIC
Laboratory Directed Research and Development (LDRD) Proposal
Electron Source Configuration
ERL accelerator review. Parameters for a Compton source
Magnetized Electron Source, LDRD
Center for Injectors and Sources
R. Suleiman and M. Poelker September 29, 2016
PIs: Riad Suleiman and Matt Poelker
November 14, 2008 The meeting on RIKEN AVF Cyclotron Upgrade Progress report on activity plan Sergey Vorozhtsov.
November 7, 2008 The meeting on RIKEN AVF Cyclotron Upgrade Progress report on activity plan Sergey Vorozhtsov.
Test of Booster at UITF Reza Kazimi (12/12/18)
MEBT1&2 design study for C-ADS
Physics Design on Injector I
CEBAF Pulsed Operation for JLEIC Electron Injection
PIs: Riad Suleiman and Matt Poelker
小型X線源の性能確認実験計画 高輝度・RF電子銃研究会 広島大学 高エネルギー加速器研究機構 浦川順治
Injector for the Electron Cooler
Update on ERL Cooler Design Studies
Transfer Line for EIC.
Technical challenges for forming the double intensity section of JLEIC ion beam Jiquan Guo.
MEIC New Baseline: Part 7
Comments to the Report of the Community Review of EIC Accelerator R&D for the Office of Nuclear Physics, February 13, 2017 (60 pages) By Haipeng Wang,
Cooler Ring Design Status - July 2017
HE-JLEIC: Do We Have a Baseline?
Generation of Magnetized Bunched Electron Beam for MEIC Cooler
Presentation transcript:

Andrew Hutton Concept suggested independently by Haipeng Wang “Straight” Merger Andrew Hutton Concept suggested independently by Haipeng Wang

Straight Merger with No Bending of Low Energy Beam Recirculated Beam Injected Beam Injector Cryomodule Septum Magnet RF Separator with Superposed Magnetic Field ERL Cryomodule

Concept (1) Use an RF Separator to separate the injected beam from the recirculating beam Immerse the RF Separator in a DC magnetic field Arrange timing and relative amplitudes so that the injected beam is not deflected Bunches are at maximum of RF deflection – bunch center has zero slope This means that the kick seen by the recirculated beam is doubled Needs to be sufficient to provide adequate separation at the septum

Waveforms Injected Bunch Recirculated Bunch

Concept (2) Use an RF Separator to separate the injected beam from the recirculating beam Immerse the RF Separator in a DC magnetic field Arrange timing and relative amplitudes so that the injected beam is not deflected This means that the kick seen by the recirculated beam is doubled Bunches are at maximum of RF deflection – bunch center has zero slope Needs to be sufficient to provide adequate separation at the septum The injector beam and the recirculating beam are further separated by a septum magnet Injected beam sees zero field Recirculating field sees deflecting field to provide adequate separation at the last injector cryomodule

Hardware – RF Separator Example: CEBAF 500 MHz separator cavity Provides a kick of >15 mrad for a 55 MeV beam using 3.5 kW RF power The magnetic field adds an equal kick Field ~100 G Total kick for 55 MeV beam is >30 mrad Assume a drift length of 2 meter Separation at the septum is >60 mm Aperture of CEBAF RF separator is 30mm Injector beam is large, but not deflected Recirculating beam is deflected ~18 mm within separator Needs more aperture at downstream end for recirculated beam

Deflection by CEBAF 499 MHz RF Separator Deflection of 55 MeV beam ≈ 15 mrad Deflection of 5 MeV beam ≈ 170 mrad Mike Spata (private communication)

Separation at Septum Separation of 60 mm accommodates halo and misalignments 60 mm 2” OD 2” OD 10 mm

Curvature of Injected Bunch (Banana effect) RF deflection of bunch center ≈170 mrad Assume 952 MHz RF separator (maximum curvature) Wavelength = 31.5 cm Bunch length = ±1 cm RF deflection at bunch ends = 170 cos (2𝛑/31.5) mrad = 170 x 0.98 = 166.6 mrad Maximum deviation at bunch ends = 170 x .02 mrad = 3.4 mrad This can be reduced by: Adjusting the dipole field to be centered on the “banana” Gains a factor of 2 Using a lower frequency Deviation is proportional to (frequency)2 Using a second structure upstream with a phase separation of 𝛑 Will need to be rotated because of the magnetization of the beam

Example of Alternate RF Separator Cavity (Cornell) https://www.classe.cornell.edu/rsrc/Home/Research/SRF/2010/Deflecting_cavity.pdf Kick is too weak for this use Try reducing aperture?

Septum Magnet The septum magnet must bend the 55 MeV beam so that it misses the Injector Cryostat ~ 50 cm Assume a drift of 1.5 meter – this means a bend angle of 17° Assume the EMMA Septum The septum length is ~8.2 cm EMMA Septum Provides 65°-70° at 10 – 20 MeV Provides 25° at 55 MeV 55 MeV EMMA Septum is acceptable as is

Timing The injected and recirculated bunches should be separated by 5.5 wavelengths inside the 952 MHz ERL Then phase of the RF Separator should be set for the injected beam The length of the arcs needs to be (n + ½) λ for energy recovery The phase of the separator is then automatically correct for the recirculated beam There is no additional requirement for the position of the RF Separator

Total Length of Merger Start from ERL cryostat end Diagnostic = 20 cm RF Septum = 60 cm Drift distance = 200 – (60/2) = 170 cm Could include diagnostics and/or solenoid for focusing Septum = 10 cm Drift distance = 150 – (10/2) = 145 cm Injector cryostat end Total = 425 cm, about ½ of FEL merger (cryostat-to-cryostat)

Test of Concept “I have been impressed with the urgency of doing. Knowing is not enough; we must apply. Being willing is not enough; we must do.” Leonardo da Vinci

Gun Test Stand Status and Plans Riad, Matt and Carlos have built a test stand which is now routinely delivering a 4.5 mA magnetized beam At this time, there is no RF structure, the gun is producing DC beam Lasers are being developed to provide bunches at a tunable RF frequency Diode laser up to 100 pC/bunch Mode-locked laser up to 1 nC/bunch They will then test the gun at different bunch charge and total beam current to try and separate the two effects on beam quality Will take a few months

“Straight” Merger at the Gun Test Stand Concept: install the spare CEBAF RF Separator in the GTS line with a superposed magnetic field Goal: evaluate the effect on a magnetized beam and study the banana effect Basic set-up: RF Separator and amplifier exist at the lab; diagnostics exist on the GTS line, most of the other equipment can be found at the lab RF Separator could provide ~6 times the kick to the magnetized beam than the proposed merger due to low beam energy Should be enough to see possible effects By changing relative phase of laser and RF separator, banana effect can be enhanced Should be able to see onset of effects Would be an excellent thesis project!

“Straight” merger at the Gun Test Stand Installation of a test of the ”straight” merger would be possible in FY18 Requires Detailed layout (Reza Kazimi ?, Joe Gubeli) Simulations (Reza Kazimi ?) An existing spare CEBAF 500 MHz separator cavity (Mark Wissmann) Building a dipole coils around the separator (Kevin Jordan) Installing separator and dipole coils on a GTS girder An existing 500W, 499 MHz RF SSA (Solid State Amplifier) (John Musson) Magnet power supply (borrowed) Stands for RF Separator and magnet Installation labor Operation for ~1 month to evaluate the effect of the RF separator/dipole on magnetized beam quality

Slide added after the Presentation In the discussion following the presentation, Haipeng Wang pointed out that the bunches from the 300 kV gun are non-relativistic and are not matched to the existing 499 MHz CEBAF RF Separator I had missed this point in my initial design of the experiment Further discussions led to the following conclusions: The relativistic beta value of 300 kV electrons is 0.777 It is expected that for this beta value, the efficiency of the RF Separator would be reduced, but would still produce a large enough kick to make a valid test Haipeng will calculate the expected reduction for the existing cavity This caveat will not be important for a separator specifically designed for the merger which should be optimized for deflection of a 55 MeV beam

Vision Install RF Separator/Dipole at GTS (December 2017?) Test with low-power laser (~100 pC/bunch) Wait for high-power laser to be built Test with high-power laser (~1 nC/bunch) (July 2018?) Design new LERF merger using existing hardware as much as possible Phase 1 includes only the low energy beam “Straight” merger would be one of the possible merger options Choose the most promising Seek funding for new LERF merger (Manouchehr, LDRD) Install LERF merger with magnetized gun (FY19?) Install diagnostics in zone 3 Measure performance of beam out of the gun/booster(?)/merger/cryomodule Seek funding for completion of merger (FY20?) Phase 2 includes the recirculated beam Evaluate performance at highest bunch charge obtainable in (FY20?)