RF 1/33 ALBA RF system why, how and other questions Francis Perez.

Slides:



Advertisements
Similar presentations
8th ESLS RF Meeting – September 2004 RF System 1/23 Storage Ring RF System F. Perez.
Advertisements

Beam Dynamics in MeRHIC Yue Hao On behalf of MeRHIC/eRHIC working group.
Proton / Muon Bunch Numbers, Repetition Rate, RF and Kicker Systems and Inductive Wall Fields for the Rings of a Neutrino Factory G H Rees, RAL.
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.
1 BROOKHAVEN SCIENCE ASSOCIATES NSLS-II ASAC-2007, April. 23, 2007 Injection System with a Booster in Separate Tunnel T. Shaftan for the NSLS-II team.
Damping ring K. Ohmi LC Layout Single tunnel Circumference 6.7 km Energy 5 GeV 2 km 35 km.
KAGEYAMA, T. Open Meeting for Proto-Collaboration March 19, 2008.
SESAME Storage Ring RF-System
Thomas Roser Snowmass 2001 June 30 - July 21, MW AGS proton driver (M.J. Brennan, I. Marneris, T. Roser, A.G. Ruggiero, D. Trbojevic, N. Tsoupas,
DORIS - 2 GeV Experiences in 2011 Olympus Collaboration Meeting April 27th, 2011 F.Brinker.
X-ray Booster IR Linac Harmonic RF RF Systems for NSLS-II J. Rose, A. Blednykh, N. Towne With help from many others at BNL and other institutions.
Eric Prebys, FNAL.  We consider motion of particles either through a linear structure or in a circular ring USPAS, Knoxville, TN, Jan , 2014 Lecture.
Experimental Study of the Inductance of a Toroidal Ferrite Core at High frequencies Michelle Walker North Carolina A&T State University Supervisor: Dave.
RF particle acceleration Kyrre N. Sjøbæk * FYS 4550 / FYS 9550 – Experimental high energy physics University of Oslo, 26/9/2013 *k.n.sjobak(at)fys.uio.no.
The LHC: an Accelerated Overview Jonathan Walsh May 2, 2006.
BEPCII Transverse Feedback System Yue Junhui IHEP , Beijing Sep 17 th, 08IMAC.
Proposals for conceptual design of the CLIC DR RF system at 2 GHz 20/10/2010 A.Grudiev.
3 GeV,1.2 MW, Booster for Proton Driver G H Rees, RAL.
June 14th 2005 Accelerator Division Overview of ALBA D. Einfeld Vacuum Workshop Barcelona, 12 th -13 th September 2005 General 10 th September 2005.
Preliminary design of SPPC RF system Jianping DAI 2015/09/11 The CEPC-SppC Study Group Meeting, Sept. 11~12, IHEP.
June 14th 2005 Accelerator Division Overview of ALBA D. Einfeld Vacuum Workshop Barcelona, 12 th -13 th September 2005 General 10 th September 2005.
SESAME STORAGE RING RF-SYSTEM SESAME-TAC meeting Nov.2012 SESAME SR RF System – Darweesh FOUDEH.
EDM2001 Workshop May 14-15, 2001 AGS Intensity Upgrade (J.M. Brennan, I. Marneris, T. Roser, A.G. Ruggiero, D. Trbojevic, N. Tsoupas, S.Y. Zhang) Proton.
05/05/2004Cyrille Thomas DIAMOND Storage Ring Optical and X-ray Diagnostics.
Cavities Auto Recovery with Beam RF&Linac Section - ALBA Accelerators Division Francis Perez Angela Salom.
13 th April 2007FFAG 07 Carl Beard EMMA RF System Carl Beard, Emma Wooldridge, Peter McIntosh, Peter Corlett, Andy Moss, James Rogers, Joe Orrett ASTeC,
PROTON LINAC FOR INDIAN SNS Vinod Bharadwaj, SLAC (reporting for the Indian SNS Design Team)
February 2010 ALBA Synchrotron Light Source Francis Perez.
Overview of Booster PIP II upgrades and plans C.Y. Tan for Proton Source group PIP II Collaboration Meeting 03 June 2014.
BEPCII Transverse Feedback System Yue Junhui Beam Instrumentation Group IHEP , Beijing.
FNAL 8 GeV SC linac / HINS Beam Dynamics Jean-Paul Carneiro FNAL Accelerator Physics Center Peter N. Ostroumov, Brahim Mustapha ANL March 13 th, 2009.
Review 09/2010 page RF System for Electron Collider Ring Haipeng Wang for the team of R. Rimmer and F. Marhauser, SRF Institute and Y. Zhang, G. Krafft.
WG2 (Proton FFAG) Summary G.H. Rees. Proton Driver Working Group  Participants: M. Yashimoto, S. Ohnuma, C.R. Prior, G.H. Rees, A.G. Ruggiero  Topics:
Bunch Separation with RF Deflectors D. Rubin,R.Helms Cornell University.
Comparison of Fermilab Proton Driver to Suggested Energy Amplifier Linac Bob Webber April 13, 2007.
Canadian Light Source Commissioning Progress CLS Annual Users Meeting –
The Introduction to CSNS Accelerators Oct. 5, 2010 Sheng Wang AP group, Accelerator Centre,IHEP, CAS.
Eric Prebys, FNAL.  We consider motion of particles either through a linear structure or in a circular ring USPAS, Hampton, VA, Jan , 2015 Longitudinal.
Digital LLRF: ALBA and Max-IV cases RF&Linac Section - ALBA Accelerators Division Angela Salom.
ALBA RF Systems Francis Perez.
Jørgen S. Nielsen Center for Storage Ring Facilities (ISA) Aarhus University Denmark ESLS XXIII (24-25/ ), ASTRID2 facility 1.
Neutrino Factory by Zunbeltz, Davide, Margarita, Wolfgang IDS proposal.
A CW Linac scheme for CLIC drive beam acceleration. Hao Zha, Alexej Grudiev 07/06/2016.
Operation Status of the RF Systems and Taiwan Photon Source
Bunch Shape Monitor for HINS Wai-Ming Tam Project X Collaboration Meeting September 11, 2009.
The LEP Superconducting RF system has reached its maximum configuration of 288 four-cell cavities powered by 36 klystrons in In 2000, this system,
PETRA III at DESY Hamburg/Germany
How does a klystron work? TE-MPE Section Meeting Karolina Kulesz
Considerations on RF systems of SPPC collider and its injector chain
Cavity-beam interaction and Longitudinal beam dynamics for CEPC DR&APDR 宫殿君
Part2: Cavities and Structures
Bunch Separation with RF Deflectors
EffiCAS Efficient Facility for Ions at CAS
Beam Loading Effect in CEPC APDR
Performance Degradation cERL Injector Cryomodule
CEPC Injector Damping Ring
LHC (SSC) Byung Yunn CASA.
Part2: Cavities and Structures
A Design Study of a Compressor ring for
Jim Clarke ASTeC Daresbury Laboratory March 2006
PETRA IV System design concept Old and new machine
Status of CTC activities for the Damping rings
Status and New Developments of ALBA RF Systems
Harmonic RF systems for ESRF-EBS - Preliminary considerations -
Status and New Developments of ALBA RF Systems
CEPC SRF Parameters (100 km Main Ring)
Parameters Changed in New MEIC Design
RF Parameters for New 2.2 km MEIC Design
Used PEP-II 476 MHz Cavities for MEIC Collider Rings
RF Parameters for New 2.2 km MEIC Design
Presentation transcript:

RF 1/33 ALBA RF system why, how and other questions Francis Perez

RF 2/33 Contents WHY? HOW? WHICH? Other questions

RF 3/33 WHY? we need a RF System to: –accelerate the electron beam to high speeds (~c) / high energy –restore the energy loss via synchrotron radiation of the stored e - beam –provide a stable energy bucket to ensure a long lifetime

RF 4/33 WHY? To accelerate the electron beam to high speeds (~c) / high energy –1st in the LINAC: 90 keV to 100 MeV –2nd in the BOOSTER: 100 MeV to 3 GeV

RF 5/33 WHY? To restore the energy loss via synchrotron radiation of the stored e - beam V = E eff. gap 400 mA 1.3 MeV/turn 520 KW Energy Time T revolution 881 ns Cavity Voltage 3.0 GeV 1.3 MeV 1.3 MV

RF 6/33 WHY? provide a large stable energy bucket to ensure a long lifetime of the stored e - beam High Voltage Low Voltage For ALBA SR:3.6 MV 3% Energy Aceptance

RF 7/33 HOW? inside the RF cavities an electromagnetic field is stored –and we will make use of: –to create a force that will accelerate the electrons create a stable well potential F = q E

RF 8/33 HOW? The electrons are moving and the e-m field oscillating F = q E E(s,t) = E 1 (s).E 2 (t) at the cavities elsewhere Electrons are bunched: ~10 mm long 600 mm apart

RF 9/33 HOW? in the LINACto 100 MeV 70 MW pulsed 3.5  s Which provides effective ~100 MV of accelerating voltage for the e - beam in ~10 meters

RF 10/33 HOW? in the BOOSTERto 3 GeV 1 cavity (5 cells) 60 kW cw to produce 1.2 MV the e- beam will be accelerated in ~150 ms, 3 times per second

RF 11/33 HOW? in the SRat 3 GeV N cavities to provide 520 kW for the beam to provide 3.6 MV 3% energy acceptance

RF 12/33 WHICH Cavity? NC 100 MHz MAXlab NC 180 MHz BNIP SC 352 MHz SOLEIL NC 500 MHz ELETTRA NC 500 MHz EU SC 500 MHz CORNELL

RF 13/33 ELETTRA Total Voltage3.6MV No Cells/IPC6 Type of cavitync Voltage / cell600kV R shunt 3.4MW Cavity power53kW Beam power/cav87kW IPC power140kW Amplifier Power160kW Total Power960kW

RF 14/33 EU project Total Voltage3.6MV No Cells/IPC6 Type of cavitync Voltage / cell600kV R shunt 3.0MW Cavity power60kW Beam power/cav87kW IPC power147kW Amplifier Power160kW Total Power960kW

RF 15/33 SC CORNELL Total Voltage3.6MV No Cells/IPC2 Type of cavitysc Voltage / cell1800kV R shunt 4500MW Cavity power0kW Beam power/cav260kW IPC power260kW Amplifier Power300kW Total Power600kW

RF 16/33 Which cavity? (1) ELETTRA(2) EU(3) CORNELL DC POWER2.5 MW2.6 MW2.1 MW WATER COOLING 220 m 3 /h230 m 3 /h140 m 3 /h Cavity Wall Dissipation Refrigerator Turbines

RF 17/33 (1) ELETTRA(2) EU(3) CORNELL SPACE2 x 2.9 m 2 x 3.3 m 3 cavities in one 4 m straight 1 cavity in one 4 m straight COST ESTIMATION 9.3 M€9.9 M€ +600 k€ 10.6 M€ k€ 6 x 1.55 M€6 x 1.65 M€2 x 5.3 M€ Which cavity?

RF 18/33 COST DIFFERENCES (1) ELETTRA (2) EU(3) CORNELL INVESTMENT0+600 k€+1300 k€ RUNNING (10y) (6000 h/year, 0.1 €/kWh) k€+3000 k€0 MAN POWER (10y) (1.5 man/year) k€ TOTAL+2400 k€+3600 k€+2200 k€ COST DIFFERENCE OVER 10 YEARS +200 k€+1400 k€0 SPACE, SERVICES and COST are NOT DECISION FACTORS Which cavity?

RF 19/33 HOM instabilities A RF cavity has more than just the fundamental resonance frequency at 500 MHz HOMs Other questions

RF 20/33 HOM instabilities When a multiple of the revolution frequency „hits“ a HOM a resonance condition arise and a instability is created. f HOM = n f rev (plus sidebands) StableInstable

RF 21/33 Comparison: Longitudinal HOMs Stability threshold for 400 mA Cavity temperature tuning should reduce the ELETTRA HOMs impedances

RF 22/33 Comparison: Transverse HOMs Stability threshold for 400 mA Stability because the cavities are in a low beta section (2 m)

RF 23/33 WHICH CAVITY? SC assures beam stability, but recovery time after failure is longer… NC has shorter recovery time after failure, but needs extra care to assure beam stability Beam stability vs. Beam availability

RF 24/33 Cavities Klystron Cooling Rack HVPS NC RF

RF 25/33 Cavity Gas reservoir Dewar Turbines Valve Box SC RF

RF 26/33 Total Voltage3,6MV Number Cells6 Voltage per cav600kV Shunt Impedance3,4Mohm Cavity power53kW Beam power / cell87kW IPC power140kW Amplifier Power160kW Number Amplifiers6 RF Amplifier Other questions NC

RF 27/ kW amplifier (IOTs) CAVITY HVPS + Amplifier 160 kW CAVITY … x 6 HVPS + Amplifier 160 kW Other questions RF Amplifier NC

RF 28/33 Total Voltage3,6MV Number Cells2 Voltage per cav1800kV Shunt Impedance4500Mohm Cavity power0,4kW Beam power / cell260kW IPC power260kW Amplifier Power>280kW Number Amplifiers2 SC Other questions RF Amplifier

RF 29/ kW amplifier (klystron/IOT) CAVITY HVPS +Amplifier 300 kW CAVITY HVPS + Amplifier 300 kW SC Other questions RF Amplifier x 2

RF 30/ kW Amplifier: Klystron vs IOTs combination

RF 31/ kW Amplifier IOT combination via a cavity combiner: 80 HVPS CAVITY 300 kW

RF 32/33 Cavity combiner We want to produce a power prototype E. Wooldridge, ASTeC

RF 33/33 SUMARY RF is needed at: –LINAC turn key system –BOOSTER 5 cell cavity, 60 kW –Storage Ring NC vs SC under discussion Klystron vs IOTs Cavity combiner prototype