Energy (ILC) and Intensity (Project X) SRF Cavity Needs

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Presentation transcript:

Energy (ILC) and Intensity (Project X) SRF Cavity Needs C.M. Ginsburg (FNAL) SRF Materials Workshop Jefferson Lab July 16-17, 2012

International Linear Collider ILC RDR ILC Specifications Initial center-of-mass energy up to 500 GeV, upgradeable to 1 TeV Ability to scan in energy between 250 and 500 GeV Integrated luminosity in the first four years 500 fb-1 at 500 GeV Peak luminosity 2 x 1034 cm-2 s-1, 75% duty factor e- e+ This design information is from the ILC Reference Design Report which was released last month. Main Linac Two 11-km linacs, one for electrons and one for positrons Accelerate from injected energy of 15 GeV to the final beam energy of 250 GeV ~16000 1.3 GHz superconducting RF cavities, operating at average gradient 31.5 MV/m CMGinsburg (FNAL) SRF Materials Workshop 16.Jul.2012

Primary design criteria ILC: SRF Cavities Primary design criteria Maximum gradient in shortest distance Minimize cost per cavity (or per cryomodule) TESLA shape was chosen as baseline Epeak/Eacc = 2.0 Bpeak/Eacc = 4.26 mT/(MV/m) Cavity performance specification vertical (qualification) test: 35 MV/m and Q0>0.8E10 operation: 31.5 MV/m and Q0>1E10 Required cavity processing Electropolishing, HPR, class-10 cleanroom assembly CMGinsburg (FNAL) SRF Materials Workshop 16.Jul.2012

ILC: Production Yields 100 100 KILC 2012 2nd pass KILC 2012 1st pass Yield [%] Yield [%] >25 >30 >35 >25 >30 >35 Max gradient [MV/m] Max gradient [MV/m] Electropolished 9-cell ILC cavities built by established vendors Processed by established labs: JLab/DESY/KEK 1st-pass cavity yield at >35 MV/m is (31 +- 7) % 2nd-pass cavity yield at >35 MV/m is (57 +- 8)% CMGinsburg (FNAL) SRF Materials Workshop 16.Jul.2012

ILC: Beyond the Baseline Studies 50 MV/m Several instances of this gradient level with different cell shapes trade off lower Bpeak/Eacc = ~3.5 mT/(MV/m) for higher Epeak/Eacc ~2.2 Avoiding field emission (even) more important Reduce cost Hydroformed cavities? (shapability, Nb properties) Large grain material? (surface roughness, earing, BCP only) Looser material specs? (tantalum content, targeted inspection) Better performance after first pass (Tumbling? Better diagnostic tools?) CMGinsburg (FNAL) SRF Materials Workshop 16.Jul.2012

Project X at Fermilab High-power proton beam with flexible beam formats delivered simultaneously to multiple users 3 MW at 3 GeV Rare process experiments with kaons, muons, nuclei Extraction of up to 0.5 mA at 1 GeV is possible 0.080-0.200 MW at 8 GeV Rare process experiments, neutrinos 2 MW at 60-120 GeV Long-baseline neutrino experiments Path toward neutrino factory or muon collider CMGinsburg (FNAL) SRF Materials Workshop 16.Jul.2012

Project X Linac SRF Cavities b=0.11 b=0.22 b=0.4 b=0.61 b=0.9 325 MHz 10-160 MeV b=1.0 1.3 GHz 3-8 GeV ILC 162.5 MHz 2.1-10 MeV 650 MHz 0.16-3 GeV H- CW Pulsed Section Freq Energy (MeV) Cav/mag/CM Type HWR (G=0.11) 162.5 2.1-10 9 /6/1 Half Wave, solenoid SSR1 (G=0.22) 325 10-42 16/8/ 2 Single Spoke, solenoid SSR2 (G=0.47) 42-160 36/20/4 LB 650 (G=0.61) 650 160-460 42 /14/7 5-cell elliptical, doublet HB 650 (G=0.9) 460-3000 152/19/19 ILC 1.3 (G=1.0) 1300 3000-8000 224 /28 /28 9-cell elliptical, quad 6 cavities/CM for low-beta 650’s 8 cavities/CM for high-beta 650’s CMGinsburg (FNAL) SRF Materials Workshop 16.Jul.2012

Project X: SRF Cavities Primary design criteria Minimize power dissipation (esp. 650 MHz b=0.9) Performance challenges Requirements for Epeak and Bpeak are modest Multipacting is an issue for the complex shapes: cleanliness Power dissipation requirement on 650 MHz cavities must be optimized JLab design for b=0.61 achieved proof-of-principle Q0 in single-cells using BCP No data for b=0.9 yet, but Q0 ~2E10 in the 15-20 MV/m range, in operation, may be challenging How to optimize Q0 CMGinsburg (FNAL) SRF Materials Workshop 16.Jul.2012

General Materials Issues For any of our projects… CMGinsburg (FNAL) SRF Materials Workshop 16.Jul.2012

Features seen on an ILC cavity Cavity was light BCP’d (10-15 um) at AES 1mm before bulk EP after bulk EP at ANL/FNAL TB9AES013 CMGinsburg (FNAL) SRF Materials Workshop 16.Jul.2012

More… This cavity reached 38 MV/m! 1 2 3 TB9AES013: Pits observed in all three images, but generally enhanced by EP. Pits are not restricted to just the equator weld or the heat affected zone. 1) Optical inspection of equator weld before EP 2) Photo before electropolishing. 3) Photo after electropolishing ( ~ 120 microns removed) 1 2 3 This cavity reached 38 MV/m!

Niobium for Project X Cavities 3mm Nb sheets All surfaces are rough, were high-speed buffed Lots of inclusions, pits Indications of poor handling, e.g., Nb on Nb rub marks Deep scratches Inspection by Z.Conway, T. Reid (ANL) An SSR1 made from this material performed the best ever! CMGinsburg (FNAL) SRF Materials Workshop 16.Jul.2012

General Materials Issues What types of material flaws matter? Material cost, inspection/remediation effort, risk, etc. CMGinsburg (FNAL) SRF Materials Workshop 16.Jul.2012