Project X Cavity RF and mechanical design. T. Khabiboulline, FNAL/TD/SRF

Similar documents
Progresses on China ADS Superconducting Cavities

DESIGN OF SINGLE SPOKE RESONATORS FOR PROJECT X*

DESIGN AND BEAM DYNAMICS STUDIES OF A MULTI-ION LINAC INJECTOR FOR THE JLEIC ION COMPLEX

Completion of the first SSR1 cavity for PXIE

SRF Advances for ATLAS and Other β<1 Applications

A 3 GHz SRF reduced-β Cavity for the S-DALINAC

5.5 SNS Superconducting Linac

Design of the 352MHz, beta 0.50, Double- Spoke Cavity for ESS

Current Industrial SRF Capabilities and Future Plans

PIP-II Superconducting RF Linac Status and Challenges" Leonardo Ristori! ICEC-ICMC Conference, New Delhi! 9 March 2016!!

SUPERCONDUCTING PROTOTYPE CAVITIES FOR THE SPALLATION NEUTRON SOURCE (SNS) PROJECT *

Overview of ERL Projects: SRF Issues and Challenges. Matthias Liepe Cornell University

Status of the superconducting cavity development at RISP. Gunn Tae Park Accelerator division, RISP May 9th. 2014

DESIGN STUDY OF A 176 MHZ SRF HALF WAVE RESONATOR FOR THE SPIRAL-2 PROJECT

Cornell ERL s Main Linac Cavities

Advances in CW Ion Linacs

Advance on High Power Couplers for SC Accelerators

CEBAF waveguide absorbers. R. Rimmer for JLab SRF Institute

Experience with 3.9 GHz cavity HOM couplers

SUPERCONDUCTING RESONATORS DEVELOPMENT FOR THE FRIB AND ReA LINACS AT MSU: RECENT ACHIEVEMENTS AND FUTURE GOALS

CONICAL HALF-WAVE RESONATOR INVESTIGATIONS

LOW BETA CAVITY DEVELOPMENT FOR AN ATLAS INTENSITY UPGRADE

Raja Ramanna Center for Advanced Technology, Indore, India

Structures for RIA and FNAL Proton Driver

Superconducting RF cavities activities for the MAX project

Cavity development for TESLA

Superstructures; First Cold Test and Future Applications

Dong-O Jeon Representing RAON Institute for Basic Science

Physics Requirements Document Document Title: SCRF 1.3 GHz Cryomodule Document Number: LCLSII-4.1-PR-0146-R0 Page 1 of 7

CHALLENGES IN ILC SCRF TECHNOLOGY *

The European Spallation Source. Dave McGinnis Chief Engineer ESS\Accelerator Division IVEC 2013

Third Harmonic Superconducting passive cavities in ELETTRA and SLS

3.9 GHz work at Fermilab

REVIEW OF HIGH POWER CW COUPLERS FOR SC CAVITIES. S. Belomestnykh

DEVELOPMENT OF A BETA 0.12, 88 MHZ, QUARTER WAVE RESONATOR AND ITS CRYOMODULE FOR THE SPIRAL2 PROJECT

Engineering Challenges and Solutions for MeRHIC. Andrew Burrill for the MeRHIC Team

Main Injector Cavity Simulation and Optimization for Project X

The TESLA Linear Collider. Winfried Decking (DESY) for the TESLA Collaboration

Couplers for Project X. S. Kazakov, T. Khabiboulline

RF Design of Normal Conducting Deflecting Cavity

Crab Cavities for FCC

ADVANCES IN CW ION LINACS*

COUPLER DESIGN CONSIDERATIONS FOR THE ILC CRAB CAVITY

Triple-spoke compared with Elliptical-cell Cavities

LOW-β SC RF CAVITY INVESTIGATIONS

Resonant Excitation of High Order Modes in the 3.9 GHz Cavity of LCLS-II Linac

Tuning systems for superconducting cavities at Saclay

HOM/LOM Coupler Study for the ILC Crab Cavity*

CURRENT INDUSTRIAL SRF CAPABILITIES AND FUTURE PLANS

HIGH Q CAVITIES FOR THE CORNELL ERL MAIN LINAC

Review of New Shapes for Higher Gradients

Crab Cavity Systems for Future Colliders. Silvia Verdú-Andrés, Ilan Ben-Zvi, Qiong Wu (Brookhaven National Lab), Rama Calaga (CERN)

BESSY VSR: SRF challenges and developments for a variable pulse-length next generation light source

Low and Medium-β Superconducting Cavities. A. Facco INFN-LNL

Development of Superconducting CH-Cavities for the EUROTRANS and IFMIF Project 1

THE U. S. RIA PROJECT SRF LINAC*

SC Cavity Development at IMP. Linac Group Institute of Modern Physics, CAS IHEP, Beijing,CHINA

DEVELOPMENT, PRODUCTION AND TESTS OF PROTOTYPE SUPERCONDUCTING CAVITIES FOR THE HIGH BETA SECTION OF THE ISAC-II HEAVY ION ACCELERATOR AT TRIUMF

Report of working group 5

STATE OF THE ART OF MULTICELL SC CAVITIES AND PERSPECTIVES*

LORENTZ FORCE DETUNING ANALYSIS OF THE SPALLATION NEUTRON SOURCE (SNS) ACCELERATING CAVITIES *

Third Harmonic Cavity Status

Aurélien Ponton. First Considerations for the Design of the ESS Cryo-Modules

Motivation: ERL based e linac for LHeC

RENASCENCE * PERFORMANCE AND PROBLEMS ON FIRST TEST Feedthrough leaks sub 70 K. End group quenching

Accelerator R&D for CW Ion Linacs

Commissioning of the ALICE SRF Systems at Daresbury Laboratory Alan Wheelhouse, ASTeC, STFC Daresbury Laboratory ESLS RF 1 st 2 nd October 2008

Outline. I. Progress and R&D plan on SRF cavity. II. HOM damping for low-risk and FFAG lattice erhic. III. Summary. Wencan Xu 2

Niowave s Growth and the Role of STTR in its Development

To produce more powerful and high-efficiency particle accelerator, efforts have

Superconducting RF System. Heung-Sik Kang

Snowmass WG5: Superconducting Cavities and Couplers (Draft August 12, 2005 Rong-Li Geng) Topic 1: Cavity Shape

QUARTER WAVE COAXIAL LINE CAVITY FOR NEW DELHI LINAC BOOSTER*

RF STATUS OF SUPERCONDUCTING MODULE DEVELOPMENT SUITABLE FOR CW OPERATION: ELBE CRYOSTATS

S. Ghosh On behalf of Linac, IFR, Cryogenics, RF and beam transport group members. Inter University Accelerator Centre New Delhi India

Demonstration of exponential growth and saturation at VUV wavelengths at the TESLA Test Facility Free-Electron Laser. P. Castro for the TTF-FEL team

PROJECT X: A MULTI-MW PROTON SOURCE AT FERMILAB *

HIGH POWER PULSED TESTS OF A BETA=0.5 5-CELL 704 MHZ SUPERCONDUCTING CAVITY

CLIC Power Extraction and Transfer Structure. (2004)

PERFORMANCE OF THE TUNER MECHANISM FOR SSR1 RESONATORS DURING FULLY INTEGRETED TESTS AT FERMILAB

Mechanical study of the «Saclay piezo tuner» PTS (Piezo Tuning System) P. Bosland, Bo Wu DAPNIA - CEA Saclay. Abstract

Energy Recovering Linac Issues

CAGE CAVITY: A LOW COST, HIGH PERFORMANCE SRF ACCELERATING STRUCTURE*

Thermionic Bunched Electron Sources for High-Energy Electron Cooling

Plans for the ESS Linac. Steve Peggs, ESS for the ESS collaboration

LCLS-II SRF Linac Multi-lab partnership to build CW FEL based on SRF at SLAC. Marc Ross 13 January 2014

Amit Roy Director, IUAC

The Superconducting Radio Frequency Quadrupole Structures Review

THE CRYOGENIC SYSTEM OF TESLA

High acceleration gradient. Critical applications: Linear colliders e.g. ILC X-ray FELs e.g. DESY XFEL

3.9 GHz Deflecting Mode Cavity

ERL Prototype at BNL. Work supported by Brookhaven Science Associates, LLC under Contract No. DE-AC02-98CH10886 with the U.S. Department of Energy.

Performance of Superconducting Cavities for the European XFEL. Detlef Reschke DESY for the EU-XFEL Accelerator Consortium

OVERVIEW OF THE HIGH INTENSITY NEUTRINO SOURCE LINAC R&D PROGRAM AT FERMILAB *

Low-Level RF. S. Simrock, DESY. MAC mtg, May 05 Stefan Simrock DESY

Processing and Testing of PKU 3-1/2 Cell Cavity at JLab

2008 JINST 3 S The RF systems and beam feedback. Chapter Introduction

Superconducting RF for Energy-Recovery Linacs

ASSEMBLY PREPARATIONS FOR THE INTERNATIONAL ERL CRYOMODULE AT DARESBURY LABORATORY

HIGH POWER INPUT COUPLERS FOR THE STF BASELINE CAVITY SYSTEM AT KEK

Transcription:

Project X Cavity RF and mechanical design T. Khabiboulline, FNAL/TD/SRF TTC meeting on CW-SRF, 2013

Project X Cavity RF and mechanical design T 1 High ß Low ß 0.5 HWR SSR1 SSR2 0 1 10 100 1 10 3 1 10 4 E [MeV] Project X layout The Project X Linac consist of several types of cavities with different beta 2

Section Freq. (MHz) Energy (MeV) Cav/mag/CM Gradient (MV/m) Energy Gain (MeV) Q 0 @2K (10 10 ) CM Config. CM length (m) HWR 162.5 2.1-11 8 /8/1 8.2 1.7 0.5 8 x (sc) 5.8 SSR1 325 11-38 16 /8/ 2 10 2.05 0.2 4 x (csc) 5.2 SSR2 325 38-177 35 /21/ 7 11.2 5.32 1.2 sccsccsc 6.5 LB650 650 177-480 30 /20 * / 5 16.5 11.6 1.5 ccc-fd-ccc 7.1 HB650 650 480-1000 42 / 16 / 7 17 17.6 2.0 cccccc 9.5 HB650 650 1000-3000 ProjectX Cavity RF and mechanical design 120 / 30 / 15 17 17.6 2.0 cccccccc 11.2 Transit time factor versus the ratio of the beta to the geometric beta, b/b G, for different number of cells in a cavity, n 3

Complicated beam structure in ProjectX A typical bunch structure required for muon, kaon, and nuclear experiments running in parallel at 3 GeV The beam current spectrum contains Harmonics of the bunch sequence frequency of 10.15 MHz Sidebands of the harmonics of 81.25 MHz separated by 1 MHz. 162.5 MHz beam sequence frequency. 4

Half-Wave Resonator(HWR) New donut shape drift tube has better field symmetry. HWR Cavity Design Value Frequency 162.5 MHz Optimum Beta 0.112 (b OPT ) Aperture 33 mm (diameter) L EFF = b OPT 20.7 cm R/Q 0 275 G = Q 0 R S 48 E max /E acc 4.65 B max /E acc 5.0 mt/(m V/m) Q 0 0.5 10 10 Operating Temperature 2 K RF and mechanical design of dressed cavity complete Cavity and power coupler under production. 5

SSR1 Cavity Design Value Frequency 325 MHz Optimum Beta (b OPT ) 0.222 Aperture (diameter) 30 mm L EFF = b OPT 20.5 cm R/Q 0 242 G = Q 0 R S 84 E max /E acc 3.84 B max /E acc 5.81 mt/(mv/m) Q 0 0.5 10 10 Operating temperature 2 K Single Spoke Resonator1(SSR1) 12 (2old and 10 new) cavities manufactured 10 (2 old and 8 new) cavities tested in VTS. Main issue is long time for multipactor processing 6 new cavities qualified for dressing 1 old cavity dressed, df/dp not optimized 1 old cavity tested in HTS (STC) with high Qext coupler (CW) and high power coupler (pulsed) 6

Dressing of SSR1 1 st dressed SSR1 cavity New design of Helium vessel design goal was reducing df/dp. df/dp <10 Hz/mbar is expected Transition ring welded to the 1 st cavity. Frequency shifted by -500 khz New SSR1 tuner 7

Single Spoke Resonator2 (SSR2) New design is result of compromise for ProjectX and RISP applications RF and mechanical design complete Multipactor simulations in progress Parameter Value Frequency 325 MHz β o 0.514 L eff = 2*(β o λ/2) 475. 3 mm Iris Aperture 50 mm E pk /E acc 3.53 B pk /E acc 6.25 mt/(mv/m) G 119 Ω R/Q 276 Ω Operating gain / cav 5 MeV Max Gain / cav 5.32 MeV Q 0 >8 x 10 9 df/dp < 19 Hz/mbar Operating temp 2 K 8

Low beta 650 MHz 1-cell cavity 3 JLAB β=0.6 cavities, 100mm iris with, 0 degree 3 FN AL β=0.6 cavities, 86mm iris with, 1.9 degree Different shape 650MHz cavities were simulated for multipactor properties Multipactor can be processed away 9

High beta 650 MHz 1-cell cavity 6 single cell cavities manufactured 2 cavities tested in VTS. Both tested cavities exceed design gradient and Q0. R&D ongoing to find best processing recipe for Q maximization, see A. Grassellino s talk tomorrow 10

High beta 650 MHz 5-cell cavity Original design of the dressed cavity optimized for High stiffness and mechanical resonances Low df/dp. But in other hand Too stiff for room temperature frequency and FFtuning Large load to the tuner, cavity stiffness 18 kn/mm 11

High beta 650 MHz 5-cell cavity tune-ability study F=45kN F=19kN R=134mm, push R=110mm, push Von Misses stress Von Misses stress Stiffening ring radius reduced from 134 mm to 110 mm Stresses in stiffening ring during FF tuning reduces 2 times Cavity stiffness reduced from 18 kn/mm to 7 kn/mm. 12

Dressed high beta 650 MHz 5-cell cavity optimization End Tuner Blade Tuner fixed Current 18 Proposed 7 End Stiffening Ring Radius Current: 126 mm Proposed: 110 mm Middle Stiffening Ring Radius Current: 134 mm Proposed: 110 mm Current cavity design was too stiff ~18 kn/mm Stiffening ring radius needs to get smaller to soften the cavity To keep df/dp within acceptable limits bellows radius needs to get smaller End tuner is proposed to replace the blade tuner Proposed Stiffening Ring Radius End Tuner Blade Tuner Current Stiffening Ring Radius 13

Dressed high beta 650 MHz 5-cell cavity, new design Mechanical resonances New design of helium vessel developed df/dp ~ 10 Hz/mbar (in FRS <15 Hs/mBar) Lever tuner 3D design complete 14

New high beta 650 MHz 5-cell cavity 10 ma Flat 5-th monopole pass band Larger aperture, 118 mm (was 100 mm) Wider HOM pass bands, good for higher beam current More cell to cell coupling, better field stability Increased coupling with the power coupler 15

Process single and 5-cell bare cavities Test in VTS Best high Q recipe found on single cell will be implemented HPR, EP, BCP, Centrifugal Barrel Polishing (Tumbling), heat treatments.etc. Continue fabrication of prototypes Lever Tuner Helium vessels Assembly and welding fixtures Dress 5-cell cavity VTS tests Room temperature tests Mechanical test of tuner(s) HTS tests Assembly of 6 best cavities in 1 st HB cryostat 16

RF Splitters Two-cell deflecting mode cavity The first will split the beam buckets into two equal parts for bunch frequencies of 162.5 MHz. This requires operations at frequencies equal to (n+1/2) 162.5 MHz The splitter in Stage 2 splits the beam with 81.25 MHz bunch into 3 parts, the frequency of this RF splitter has to be (n+1/4) 81.25 MHz Stage I II Operating frequency, MHz 406.25 426.5625 Number of cells 2 2 Optimal beta 0.87 0.92 Transverse kick, MeV 7 7 Maximal surface electric field, MV/m 36 37 Maximal surface magnetic field, mt 50.5 52 R/Q*, Ohm 485 510 G-factor, Ohm 115 115 Dimensions, mm 3 270 270 1200 260 260 1150 Aperture, mm 70 65 Preliminary RF design is proposed Helium vessel and frequency tuner development is planned 17

3-8 GeV Pulsed Linac cavity Parameter Recycler/MI Direct Injection to MI Units Frequency 1.3 1.3 GHz Loaded Q 1.e7 1.e7 RF pulse width 7.4 30 ms Cavity Gradient 25 25 MV/m Beam current 1 1 ma Repetition rate 10 10 Hz Cavity RF power 32 32 kw Cavity power +losses+regulation +EOL 50 50 kw Power per Cryomodule 400 400 kw Existing ILC cavity Needs new Power Coupler design with higher average power 18

Summary HWR production in ANL in progress SSR1 cavities fro 1 st cryomodule are manufactured and VTS tests almost complete Dressing (new design) of 1 st SSR1 cavity in progress SSR2 design modified to fit both Project X and RISP 2 designs of low beta 650 MHz single cell cavities are manufactured. JLAB design successfully tested in VTS at JLAB and FNAL. High beta 650 MHz single cell cavities are manufactured. 2 cavities tested in VTS High beta 650 MHz 5-cell (original design) 9 cavities under production. 4 of them will be delivered in June. 6 best will be used for installation in 1 st cryomodule. Mechanical design of dressed cavity with lever tuner complete New RF design of high beta 650 MHz 5-cell complete and approved for Project X 19

1. What are the design criteria for frequency, #cells, and geometric-beta choices, cell shapes? Bunch repetition frequency choice depend available technology: amplifiers, developed RF system. Accelerating cavity frequency is a harmonic of injector frequency. Odd harmonics used for acceleration of both positively and negatively charged particles. Number of cells defined by available space, field distribution stability, required β range, technology limits. Geometric beta by beam dynamics, power losses, available technology Cell shape by surface field optimization, power loss surface processing technology 2. What are the design criteria driven by beam current, emittance, LOM's, HOM's? All modes resulting to additional cryo-loading, emittance grow, beam stability should be damped 3. How predictive are HOM calculations? Manufacturing accuracy, difference on (chemical) treatment, tuning requirements 4. How predictive are 3D multipacting calculations? Current simulation tools allow to predict with good accuracy multipacting. Quantity is depend on surface preparation 5. What determines production tolerances? Forming accuracy 0.1-0.3 mm, weld shrinkage accuracy 0.1-0.2 mm 6. What level of mechanical stability (stiffness) is required to operate reliably and to maintain tuneability? Mechanical stability is compromise between desire of higher mechanical resonances and acceptable tune-ability Sensitivity to helium pressure fluctuations df/dp is not necessarily require highest stiffness 20