Coupler without copper coating S. Kazakov 11/13/2013.

Slides:



Advertisements
Similar presentations
MICE RF and Coupling Coil Module Outstanding Issues Steve Virostek Lawrence Berkeley National Laboratory MICE Collaboration Meeting October 26, 2004.
Advertisements

30 th September 2004 High Power RF Couplers James Rogers High Power RF Couplers ELSRF Daresbury Laboratory.
KCS Ongoing R&D Christopher Nantista SLAC LCWS11 Granada, Spain September 29, …… …… …… … ….
Status of the 201 MHz Cavity and Coupling Coil Module Steve Virostek Lawrence Berkeley National Laboratory MICE Video Conference March 10, 2004.
Design of Standing-Wave Accelerator Structure
Status of 325MHz coupler S. Kazakov 11/29/ MHz coupler structure.
SPIE Conference - Photonics Applications in Industry and Research, Warsaw, 30 August, The RF Power Coupler Development Program at LAL-Orsay and.
201 MHz and 805 MHz Cavity Developments in MUCOOL Derun Li Center for Beam Physics Lawrence Berkeley National Laboratory Nufact 2002 Workshop, London,
RFQ Thermal Analysis Scott Lawrie. Vacuum Pump Flange Vacuum Flange Coolant Manifold Cooling Pockets Milled Into Vanes Potentially Bolted Together Tuner.
ELECTROMAGNETIC, THERMAL, AND STRUCTURAL ANALYSIS OF RF CAVITIES USING ANSYS 2.1 GHz 3-Cell Cavity Cliff Brutus 6/15/15 Job Name: 2.1ghz_Symmetry_
Status of RFCC-Module Development Derun Li Center for Beam Physics Lawrence Berkeley National Laboratory MICE Collaboration Meeting at INFN-LNF, Frascati,
201 MHz NC RF Cavity R&D for Muon Cooling Channels
Summary of AWG7 SCRF technologies Eiji Kako Wolf-Dietrich Moeller Akira Yamamoto Hitoshi Hayano Tokyo, Nov
Materials Testing With a High-Q RF Cavity Sami Tantawi, Christopher Nantista, Valery Dolgashev, Gordon Bowden, Ricky Campisi, T. Tajima, and P. Kneisel.
ELECTROMAGNETIC, THERMAL, AND STRUCTURAL ANALYSIS OF RF CAVITIES USING ANSYS 2.1 GHz 3-Cell Cavity Cliff Brutus 7/9/15 Workbench Job Name: 2.1ghz_Symmetry_
201 MHz Cavity Status and Test Plans at MTA MICE Collaboration Meeting at RAL, UK October 22 ~ 24, 2005 Derun Li Center for Beam Physics Lawrence Berkeley.
F.E.T.S. RFQ Mechanical Design by Peter Savage 7 th January 2010.
Work toward Stainless Steel SRF Helium Vessels at Fermilab Tom Peterson (presenter), Information from Jeff Brandt, Serena Barbanotti, Harry Carter, Sergei.
Clustered Surface RF Production Scheme Chris Adolphsen Chris Nantista SLAC.
2.1GHz cavity without cell-to-cell coupling slots – 1.875” beam pipe Binping Xiao Aug
Cavity support scheme options Thomas Jones 25/06/15 to 06/07/15 1.
Study of Absorber Effectiveness in the ILC Main Linacs K. Bane, C. Nantista and C. Adolphsen SLAC, March 26, 2010 Goal: Compute the HOM monopole losses.
IHEP High Power Input Coupler Activity Report First Mini-workshop on IHEP 1.3 GHz Superconducting RF project June 10th, 2009, Beijing IHEP High Power Input.
LCLS-II Power Coupler Nikolay Solyak, Ivan Gonin, Andrei Lunin C.Adolphsen - SLAC TTC meeting, March 23-27, 2014 AWLC2014, FNAL, May 12-16,
2009/1/16-18 ILD09 Seoul 1 Notes for ILD Beam Pipe (Technical Aspect) Y. Suetsugu, KEK Parasitic loss Vacuum pressure profile Some comments for beam pipe.
Rossana Bonomi ESS Cryomodule Status Meeting, 9/1/2013.
1.3GHz Input Coupler for ILC
LCWS13, November 2013 At the University of Tokyo W.–D. Möller Status of the TTF3 RF Power Coupler.
Coupler Multipactor Studies F. Wang, B. Rusnak, C. Adolphsen, C. Nantista, G. Bowden, Lixin Ge.
56 MHz SRF Cavity Thermal Analysis and Vacuum Chamber Strength C. Pai
1 Thermal tests planning for mock-up TM0 Thermal tests planning for CLIC prototype module type 0 May 30th,
Eric Montesinos - CERN - First SPL collaboration meeting - CERN December 11th 2008 First SPL collaboration meeting Experience with the LHC Main power Coupler.
LCLS-II Couplers and Related R&D Chris Adolphsen WWFPC, CERN June 23, 2015.
Summery of the power coupler session at the LCWS13 workshop E. Kako W.-D. Möller H. Hayano A. Yamamoto All members of SCRF WG November 14, 2013.
Main features of PETS tank J. Calero, D. Carrillo, J.L. Gutiérrez, E. Rodríguez, F. Toral CERN, 17/10/2007 (I will review the present status of the PETS.
Titanium Nitride Coating by Reactive DC Magnetron Sputtering as a Multipactor Suppressor on Coupler RF Ceramic Windows Walid KAABI Anti e - Cloud Coatings-
16-17 March 2010 CERN W. Weingarten DRAFT summary. rev Review of SPL RF power couplers 16/17 March 2010 Review of SPL RF power couplers 1.
Cavity support scheme options Thomas Jones 25/06/15 1.
MAIN LINAC CRYOMODULE DESIGN REVIEW INPUT COUPLER September 5, 2012V. Veshcherevich.
13/Nov/ mm STF2 Coupler Design Content 1.Motivation 2.40mm Design 3.“Preliminary” Result by HFSS 4.“Tentative” Conclusion 5.Future.
S1 global: thermal analysis TILC09, April 19th, 2009 Serena Barbanotti Paolo Pierini.
Preparation procedure and RF processining of cERL-ML power coupler at KEK Hiroshi Sakai, Takaaki Furuya, Masato Sato, Kenji Shinoe, Kensei Umemori, Kazuhiro.
Power couplers Timergali Khabiboulline (FNAL) FNAL-LBNL meeting on NGLS April 13, 2012.
Guillaume Olry, Sébastien Bousson CNRS/IN2P3/ IPN Orsay – Paris-Sud University Experience on Spiral2 cavity cleanliness degradation during clean room assembly.
BARC’s CW Power Coupler at 325 MHz for IIFC Rajesh Kumar BARC alternate mail id:
RFQ coupler S. Kazakov 07/28/2015. Requirements: Coupler requirements Expected problems: Heating (loop, ceramic window, etc.) Multipactor Solutions: Appropriate.
Superconducting Materials Testing With a High-Q Copper RF Cavity Sami Tantawi, Valery Dolgashev, Gordon Bowden, James Lewandowski, Christopher Nantista.
R. Bonomi - SLHiPP2, Catania 3-4/5/20121 SPL Thermal Studies R. Bonomi Superconducting linacs for high power proton beams - Catania, 2012.
IFMIF Power Coupler for HWR Superconducting cavities SRF LINAC GROUP H. Jenhani 1, N. Bazin 1, P. Bosland 1, B. Branas 2, P. Brédy 1, P. Carbonnier 1,
SPS High Energy LSS5 Thermal contact & cooling aspects
Prototype Cryomodule FDR Ken Premo 21 – 22 January 2015 High Power Coupler Design.
325 MHz Superconducting Spoke Cavity Coupler status. T. Khabiboulline Power Coupler design for Superconducting Spoke cavities. Originally.
XFEL beamline loads and HOM coupler for CW
T5.2: Harmonization - Material and Component Reference
Power Couplers, HOM Couplers and Tuners for the XFEL
Power coupler at DESY & for XFEL
Axion Relics Thermal – mechanical simulation for a flange UHV 114/63 1D with copper gasket
Input coupler assembly, high power and thermal performance in S1-Global at KEK E. KAKO (KEK) 2011' Dec. 07 TTC meeting in Beijing.
Challenges of vacuum chambers with adjustable gap for SC undulators
Crab Cavity Manufacturing Readiness Meeting
Installation plan for LAB modules
FKPPL and FJPPL Joint Workshop
V. Veshcherevich Cornell University
Main Coupler R&D at DESY
High Power Couplers and… pushing the limits of SC cavities
CEPC Input Coupler Discuss 6th IHEP-KEK SCRF Collaboration Meeting
Phase II Collimators : design status
DQW HOM Update and Recent Developments
Cryomodules Challenges for PERLE
Cryomodule Design for CW Operation 3.9 GHz considerations
Presentation transcript:

Coupler without copper coating S. Kazakov 11/13/2013

Coupler for SRF cavity has to provide low RF loss and low heat flow from room temperature to cryo-temperatures. These are contradictory requirements. Traditional solutions is thin SS coated with thin Cu. Problem with Cu coating still exists: difficult to get a durable coating, difficult to get a good reproducible RRR, cupper coating increase thermo-conductivity (requires accurate control of copper layer. We would like to suggest new approach which solves this problem: without copper coating a coupler has RF loss as a pure copper and thermal conductivity as a pure SS.

Idea: No thermal contact between copper parts SS Low fields chamber Heat flows through SS only, RF loss in SS < loss in Cu Holes for pumping and washing

With some combinations of dimensions of slot and chamber: 1)RF reflections < -35 dB 2)Н-filed at SS surface < 0.25 of H-fild at Cu surface (losses at SS will be < losses at Cu) One possible configuration:

Requirements to slot, chamber dimensions: Requirements is not so strict: Slot should be small and long enough, chamber should be big enough. Examples: Rout = 20mm Rin = 4.76mm There is no multipactor for copper slot < 0.5 mm for any fields (1.3 GHz) There is no multipactor in chamber (low fields) in operating power range.

dRdZPSRbHLRefН1H2H2/H Loss in SS will be ~ (0.2)^2 *7 ~ 0.3 of loss in copper

Preliminary mechanical analyses shows that this configuration is possible. We cannot ‘close’ the slot by bending - plastic deformations start first.

T2 K10 K100 K Static, W Total (RF = 6kW, TW), W Static One-window 1.3 GHz coupler configuration Cryo-loads, RRR = 10:

1.3 GHz coupler configurations with cold window

Main question: can we clean/wash this assembly? FNAL experts opinions: there is no problem to prepare initially clean assembly. Problem is to re-clean the chamber after first test / conditionings. May be it will be difficult to blow out particles from chamber.

Demountable configuration allows to do a re-cleaning: One warm window Temperature, K2 K10 K100 K Static load, W Total (RF=6 kW, TW) Cryo-loads, RRR = 10: Brazed or bolted

Temperature2 K10 K100 K Static load, W Total (RF = 6 kW, TW) Cryo-loads, RRR = 10: Cold window, adjustable coupling

Double bellows: Or no copper bellows : Problem – multipactor in slot. CST copper (max SE ~ 2.1), multipactor range ~ 10 kW - 2 MW, TW ‘Clean’ copper (max SE ~1.4), multipactor range ~ 25 kW – 800 kW, TW 2 K load ~ 0.1 W for 6 kW RF

Sensitivity to slot size: Optimal size – 0.82mm. Simulated mm Slot matches the window and thermally decouples cold and warm parts of antenna. window Slot We can avoid SS bellows Multipactor in 0.82mm slot: CST copper (max SE ~ 2.1), multipactor range ~ 20 W W, TW ‘ Clean’ copper (max SE ~1.4), multipatir range ~ 160 W – 250 W, TW Out of operating range E-field ~ 0.18 kV/(cm*W⁰∙⁵) 400 kW -> 114 kV/cm

Adjustable coupler with cold window Compact adjustable coupler with cold window

Compact adjustable coupler with warm window(s)

“ Realistic” conceptual designs (very preliminary) Double bellows Cylindrical capacitor

Conclusions: Pros: allow to avoid copper coating of SS. Reproducibility of RRR, low static and dynamic loss (high RRR). Cons: requires high mechanical accuracy (~ mm concentricity). Cost?