Passive harmonic cavities for bunch shortening

Slides:



Advertisements
Similar presentations
Status and Future of BESSY RF BESSY II operating since 1999 Willy Wien Laboratory groundbreaking 9/2004 HoBiCaT Testfacility for sc cavities Commissioning.
Advertisements

Linear Collider Bunch Compressors Andy Wolski Lawrence Berkeley National Laboratory USPAS Santa Barbara, June 2003.
CornellVideo Talk. Dec page 1 John Byrd Experimental studies of the fast- beam ion instability in the ALS- The Sequel John Byrd Lawrence Berkeley.
S. N. “ Cavities for Super B-Factory” 1 of 38 Sasha Novokhatski SLAC, Stanford University Accelerator Session April 20, 2005 Low R/Q Cavities for Super.
Longitudinal motion: The basic synchrotron equations. What is Transition ? RF systems. Motion of low & high energy particles. Acceleration. What are Adiabatic.
Longitudinal instabilities: Single bunch longitudinal instabilities Multi bunch longitudinal instabilities Different modes Bunch lengthening Rende Steerenberg.
RF Stability Working Group Jorn Jacob (ESRF), John Byrd (LBNL) General Issues RF phase and amplitude noise –filtered by cavity and translate into timing.
DESIGN OF A 7-CELLS, HOM DAMPED, SUPERCONDUCTING CAVITY FOR THE STRONG RF FOCUSING EXPERIMENT AT DANE David Alesini, Caterina Biscari, Roberto Boni, Alessandro.
Eric Prebys, FNAL.  We consider motion of particles either through a linear structure or in a circular ring USPAS, Knoxville, TN, Jan , 2014 Lecture.
Eric Prebys, FNAL.  As you’ll show in homework, the synchrotron tune (longitudinal oscillations/turn) is generally
Future Very High Luminosity Options for PEP-II John T. Seeman For the PEP-II Team e+e- Factories Workshop October 13-16, 2003.
Beam Instability Workshop, ESRF, 13th - 15th March 2000J. Jacob / 1 Harmonic Cavities:the Pros & Cons Jörn Jacob.
BEPCII Transverse Feedback System Yue Junhui IHEP , Beijing Sep 17 th, 08IMAC.
Impedance and Collective Effects in BAPS Na Wang Institute of High Energy Physics USR workshop, Huairou, China, Oct. 30, 2012.
Preliminary design of SPPC RF system Jianping DAI 2015/09/11 The CEPC-SppC Study Group Meeting, Sept. 11~12, IHEP.
History and motivation for a high harmonic RF system in LHC E. Shaposhnikova With input from T. Argyropoulos, J.E. Muller and all participants.
1Matthias LiepeAugust 2, 2007 LLRF for the ERL Matthias Liepe.
704MHz Warm RF Cavity for LEReC Binping Xiao Collider-Accelerator Department, BNL July 8, 2015 LEReC Warm Cavity Review Meeting  July 8, 2015.
Simulation of Beam Instabilities in SPring-8 T. Nakamura JASRI / SPring-8
RF system issues due to pulsed beam in ILC DR October 20, Belomestnykh, RF for pulsed beam ILC DR, IWLC2010 S. Belomestnykh Cornell University.
Freq [GHz]Q0Q0 R/Q [Ω]±Voltage [kV]
Office of Science Harmonic RF System Technology for Electron Storage Rings Lawrence Berkeley National Laboratory John Byrd Workshop on Advanced Low Emittance.
Lecture 25 - E. Wilson - 12/15/ Slide 1 Lecture 6 ACCELERATOR PHYSICS HT E. J. N. Wilson
BEPCII Transverse Feedback System Yue Junhui Beam Instrumentation Group IHEP , Beijing.
1Matthias LiepeAugust 2, 2007 Future Options Matthias Liepe.
Aaron Farricker 107/07/2014Aaron Farricker Beam Dynamics in the ESS Linac Under the Influence of Monopole and Dipole HOMs.
RF System Specifications for Nominal and 10Hz Operation A. Gallo and R. Boni, INFN – LNF (S. Belomestnykh, BNL) RF System Specifications for Nominal and.
R.SREEDHARAN  SOLEIL main parameters  Booster and storage ring low level RF system  New digital Booster LLRF system under development  Digital LLRF.
THE DA  NE 3 RD HARMONIC CAVITY A. Gallo, with D. Alesini, R. Boni, S. Guiducci, F.Marcellini, M. Migliorati, L. Palumbo, M. Zobov.
POWER REQUIREMENTS FOR THE LHC HARMONIC CAVITIES WITH THE FULL-DETUNING SCHEME P. Baudrenghien, T. Mastoridis, CERN BE-RF 2nd LHC Harmonic Cavity meeting,
704 MHz warm cavity November 4, 2015 A.Zaltsman: SRF & warm RF components for LEReC1  A single cell 704 MHz warm cavity is used to correct the beam energy.
Second Harmonic capture in the IPNS RCS: Transition from SH to fundamental rf operation during the acceleration cycle using CAPTURE_SPC Jeff Dooling Presented.
July LEReC Review July 2014 Low Energy RHIC electron Cooling Jorg Kewisch, Dmitri Kayran Electron Beam Transport and System specifications.
BEAMLINE HOM ABSORBER O. Nezhevenko, S. Nagaitsev, N. Solyak, V. Yakovlev Fermi National Laboratory December 11, 2007 Wake Fest 07 - ILC wakefield workshop.
Eric Prebys, FNAL.  We consider motion of particles either through a linear structure or in a circular ring USPAS, Hampton, VA, Jan , 2015 Longitudinal.
TESLA DAMPING RING RF DEFLECTORS DESIGN F.Marcellini & D. Alesini.
Marcel Schuh CERN-BE-RF-LR CH-1211 Genève 23, Switzerland 3rd SPL Collaboration Meeting at CERN on November 11-13, 2009 Higher.
LIU-SPS Beam Dynamics WG E. Shaposhnikova LIU-SPS coordination meeting
Aaron Farricker 107/07/2014Aaron Farricker Beam Dynamics in the ESS Linac Under the Influence of Monopole and Dipole HOMs.
LONGITUDINAL COUPLED-BUNCH OSCILLATIONS IN THE RECYCLER RING PRESENTED BY: MUHED RANA UNIVERSITY OF MARYLAND, BALTIMORE COUNTY (UMBC), BALTIMORE, MD SUPERVISOR:
1 DR 10 Hz Repetition Rate S. Guiducci (LNF) AD&I webex, 23 June 2010.
Harmonic system for LHC
Bocheng Jiang SSRF AP group
Longitudinal impedance of the SPS
Beam based measurements
Design Fabrication and Processing Group H. Padamsee
SuperB Injection, RF stations, Vibration and Operations
Longitudinal beam parameters and stability
Physics design on Injector-1 RFQ
John Byrd Center for Beam Physics
Working group on rf and feedback
FCC-ee: coupling impedances and collective effects
News on the TMCI and SPS transverse impedance
Overview of SRF system of Ring and Linac (1)
The new 7BA design of BAPS
I Alexander Nass for the JEDI collaboration
Analysis of Multi-Turn ERLs for X-ray Sources
CEPC Main Ring Cavity Design with HOM Couplers
Accelerator R&D Results from the B-factory
Compensation of transient RF voltage using a kicker cavity
SC ISOL Linac of KoRIA Tae-Sun Park (SKKU).
Status of RF at HZB: BESSY II, MLS, bERLinPro and BESSY VSR
Lecture 6 ACCELERATOR PHYSICS HT E. J. N. Wilson
Accelerator Physics Particle Acceleration
Harmonic Cavities:the Pros & Cons Jörn Jacob
RF Parameters Calculation for JLEIC Colliders (e Ring)
Parameters Changed in New MEIC Design
RF Parameters for New 2.2 km MEIC Design
MEIC low rep-rate operation and path length
RF Parameters for New 2.2 km MEIC Design
Presentation transcript:

Passive harmonic cavities for bunch shortening John Byrd Lawrence Berkeley National Laboratory

Voltage completely reactive (I.e. 90 phase shift w.r.t beam) Basic Idea Use reactive longitudinal focussing from beam-induced voltage in a cavity Use SC cavity so that Low beam losses Higher voltages Use at RF harmonic to get larger dV/dt Try to take advantage of developments in HOM-damped higher frequency SC cavities for rings Beam induced voltage V=jI(R/Q)fr/df Voltage completely reactive (I.e. 90 phase shift w.r.t beam) Original idea inspired by Yong Ho Chin

Basic idea (cont.) Voltage is either +-pi/2 with respect to beam: shortening or lengthening the bunch Limits to harmonic number given by bunch length and by vacuum chamber. Typical for 500 MHz main RF is third harmonic.

How to shorten bunches? Increase main RF voltage Add harmonic voltage Increase number of cells Additional HOMs Additional load on low-mode feedback Increase number of klystrons Further cost (equipment and wallplug) No hardware R&D required Add harmonic voltage Sqrt(n) gain per Volt effective in longitudinal focussing SC passive cavity operates reactively: very little power dissipation Passive operation requires no external power source (I.e. beam is the power source) Significant R&D required (cryo system, cryostat, etc.) Most colliders have existing cryo for solenoid.

Harmonic RF systems (cont.) The bunch shape can be calculated from the resulting distortion of the potential well. In the bunch lengthening case, the single particle motion is highly nonlinear and a large tune spread is introduced. bunch distribution potential potential and bunch distribution for optimal lengthening. The resulting tune spread is ~the original tune.

SC bunch shortening cavity for PEP-II The harmonic voltage can be phased to add the focussing of the main RF. Since the focussing is reactive, a passive (i.e. idling) cavity can be used to generate the voltage. Using 2 SC cells (R/Q=87 Ohms,Q=2e8), proper tuning can shorten the bunches by a factor of 2.5.

Elettra/SLS/CERN/CEA Based on Soleil 352 MHz design 2-cell w/HOM damping in between cells

Bessy-II design Based on Cornell design (cavity actually test prototype) HOM damping on external ferrite loads brazed to beam pipe

Summary Seems to be a feasible alternative for providing longitudinal focussing. Requires little beam/external power Higher harmonics give extra dV/dt Large voltages achievable in SC systems Voltage adjustable with tuning Existing designs for 1500 MHz systems. Cryostat designed Includes HOM damping Effects for large rings need to be evaluated (low mode excitation.)