KCS Ongoing R&D Christopher Nantista SLAC LCWS11 Granada, Spain September 29, 2011. …… …… …… … ….

Slides:



Advertisements
Similar presentations
Breakdown Rate Dependence on Gradient and Pulse Heating in Single Cell Cavities and TD18 Faya Wang, Chris Nantista and Chris Adolphsen May 1, 2010.
Advertisements

Single-Cell Standing Wave Structures: Design
PETS components and waveguide connections CLIC Workshop 2007 David Carrillo.
5th Collaboration Meeting on X-band Accelerator Structure Design and Test Program. May 2011 Review of waveguide components development for CLIC I. Syratchev,
Lorentz force detuning measurements on the CEA cavity
Institute for Plasma Research MURI 99 Frequency Doubling Harmonic Gyro-TWT’s (development and experimental studies) We will complete the optimization of.
Design of Standing-Wave Accelerator Structure
Beam loading compensation 300Hz positron generation (Hardware Upgrade ??? Due to present Budget problem) LCWS2013 at Tokyo Uni., Nov KEK, Junji.
Demonstration of the Beam loading compensation (Preparation status for ILC beam loading compensation experiments at ATF injector in this September) (PoP.
Christopher Nantista ML-SCRF Technology Meeting July 28, 2010 REPORT.
324MHz FETS RFQ RF measurement and components By Aaron Cheng 18 December 2006.
Christopher Nantista SLAC TILC09 Tsukuba, Japan April 20, 2009.
Alessandro Cappelletti for CTF3 collaboration 5 th May 2010 RESULTS OF BEAM BASED RF POWER PRODUCTION IN CTF3.
Test Facilities Sami Tantawi SLAC. Summary of SLAC Facilities NLCTA (3 RF stations, one Injector, one Radiation shielding) – Two 240ns pulse compressor,
7.8GHz Dielectric Loaded High Power Generation And Extraction F. Gao, M. E. Conde, W. Gai, C. Jing, R. Konecny, W. Liu, J. G. Power, T. Wong and Z. Yusof.
Coupler without copper coating S. Kazakov 11/13/2013.
Christopher Nantista Chris Adolphsen SLAC TILC09 Tsukuba, Japan April 20, 2009.
Christopher Nantista ILC 2 nd Baseline Assessment Workshop (BAW-2) SLAC January 18, …… …… …… … ….
Christopher Nantista 2011 Linear Collider Workshop of the Americas (ALCPG11) University of Oregon, Eugene March 20, …… …… …… … ….
KCS Operational Issues Chris Adolphsen, Chris Nantista and Faya Wang GDE PAC Review at KEK 12/12/12.
RF Distribution Alternatives R.A.Yogi & FREIA group Uppsala University.
November LCWS08 S. Fukuda 1 KEK HLRF Status and S1- global S. FUKUDA KEK.
Test Facilities and Component Developments Sami Tantawi SLAC May 15, 2008.
Materials Testing With a High-Q RF Cavity Sami Tantawi, Christopher Nantista, Valery Dolgashev, Gordon Bowden, Ricky Campisi, T. Tajima, and P. Kneisel.
Chris Adolphsen 10/03/09 MLI and HLRF Summary. Vladimir Kashikhin.
Christopher Nantista ARD R&D Status Meeting SLAC February 3, …… …… …… … ….
Clustered Surface RF Production Scheme Chris Adolphsen Chris Nantista SLAC.
Super High-Power Microwave Semiconductor Switches S. Tantawi F. Tamura.
MVE MURI 99 Kick-off Meeting R. Barker, Technical Monitor Started 1 May 99 October 1999 Project Introduction and Motivation Millimeter-wave switches may.
Klystron Cluster RF Distribution Scheme Chris Adolphsen Chris Nantista SLAC.
Linac R&D Update May 15, L-Band Source Consists of a LLRF system (VME/Epics based), a SNS High Voltage Converter Modulator (on loan), a Thales 2104C.
Vladimir Kashikhin. FLASH Cavity Gradient Stability Comparison of beam-off measurements of pulse-to-pulse cavity gradient jitter during the flattop.
Anders Sunesson RF Group ESS Accelerator Division
Klystron Cluster RF Distribution Scheme Chris Adolphsen Chris Nantista SLAC.
1 SPL Collaboration Meeting dec 08 - WG1 Introduction First SPL Collaboration Meeting Working Group 1 High Power RF Distribution System Introduction.
Power Distribution System R&D at SLAC Christopher Nantista ILC08 Chicago, Illinois November 18,
L-band (1.3 GHz) 5-Cell SW Cavity High Power Test Results Faya Wang, Chris Adolphsen SLAC National Accelerator Laboratory
KSC Operation Control of Cavity Gradients Failure Analysis Near and Long Term R&D Effect on Beam Emittance Chris Adolphsen SLAC 9/7/2010 Going Native in.
Christopher Nantista ILC10 Beijing, China March 27, 2010.
Ding Sun and David Wildman Fermilab Accelerator Advisory Committee
TE 01 -TE 02 DLDS Elements BINP-KEK
Power Distribution System (PDS) Design and R&D Status Christopher Nantista SLAC SCRF Fermilab April 24, 2008.
Beam Loading experiment at KEK ATF ( Multi-train acceleration at KEK-ATF Injector ) KEK Masafumi Fukuda and Junji Urakawa LCWS /10/052 train acceleration.
The Design and Analysis of Multi-megawatt Distributed Single Pole Double Throw (SPDT) Microwave Switches Sami G. Tantawi, and Mikhail I. Petelin Stanford.
The NLC RF Pulse Compression and High Power RF Transport Systems Sami G. Tantawi, G.Bowden, K.Fant, Z.D.Farkas, W.R.Fowkes J.Irwin, N.M.Kroll, Z.H.Li,
Evaluation of the TE 12 Mode in Circular Waveguides for Low-Loss High Power Transportation Sami G. Tantawi, C. Nantista K. Fant, G. Bowden, N. Kroll, and.
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.
Microwave Devices.
KCS and RDR 10 Hz Operation Chris Adolphsen BAW2, SLAC 1/20/2011.
Status of high gradient experiments at Nextef Kazue Yokoyama, Toshiyasu Higo, Yasuo Higashi, Shuji Matsumoto, Shigeki Fukuda Accelerator Laboratory, KEK.
KCS Main Waveguide Testing Chris Adolphsen Chris Nantista and Faya Wang LCWS12 Arlington, Texas October 25, 2012.
SPL waveguide distribution system Components, configurations, potential problems D. Valuch, E. Ciapala, O. Brunner CERN AB/RF SPL collaboration meeting.
HLRF R&D Towards the TDR Christopher Nantista ML-SCRF Webex meeting June 29, 2011.
Summary of Relative RF Distribution Costs with Gradient Considerations (Work in Progress) Chris Adolphsen SLAC.
Dmitry Gudkov Phase correction of the CLIC TBM in CLEX Dmitry Gudkov Wilfrid Farabolini.
Power couplers Timergali Khabiboulline (FNAL) FNAL-LBNL meeting on NGLS April 13, 2012.
Nextef status and expansion plans Shuji Matsumoto for KEK Nextef Group /5/51 4th X-band Structure Collaboration Meeting, CERN.
Superconducting Materials Testing With a High-Q Copper RF Cavity Sami Tantawi, Valery Dolgashev, Gordon Bowden, James Lewandowski, Christopher Nantista.
Christopher Nantista SLAC Project X Workshop November 12, 2007 Fermilab.
Advancements on RF systems D. Alesini (LNF-INFN) Quinto Meeting Generale Collaborazione LI2FE, Frascati 15-16/03/2011.
ILC High Power Distribution
Klystron Cluster System (KCS)
Manipulating RF phase and amplitude at high power level.
Klystron Cluster System Development
A frequency choice for the SPL machine: Impact on hardware
Chris Adolphsen Sergei Nagaitsev
Application of the moderate peak power (6 MW) X-band klystron’s cluster for the CLIC accelerating structures testing program. I. Syratchev.
12 GHz High Power RF components requirements for CEA activities
Sub – 1 Ohm Broadband Impedance Matching Network
Instability measurement plans at ATF
Presentation transcript:

KCS Ongoing R&D Christopher Nantista SLAC LCWS11 Granada, Spain September 29, …… …… …… … ….

Where We Are An 11.5 m prototype run of TE 01 -mode circular waveguide has been tested in resonant-line mode, using a CTO as an input coupler, up to ~300MW TW equivalent peak fields (~75MW each way SW). After addressing a flange gap problem, we achieved stable operation at ~18psig pressurization.

What’s Next (1) Transmission Test: We are installing our second CTO at the far end of the line, replacing the shorting plate. Both CTO’s will be fitted with end caps of the proper depth to make them launchers (i.e. designed for full coupling), and high-power loads will be installed on the rectangular outputs of the end CTO. The input match will be measured, followed by high-power running up to ~4.2MW available from our Thales klystron. Transmission and reflection will be measured with directional couplers at the input and output. Tests will be repeated with a 1/4-wave spacer inserted in the pipe. If necessary, NWA cold tests of the CTO’s back-to-back can be repeated, w/ & w/o spacer, to verify tuning of the shorting caps for optimized transmission.

What’s Next (2) Breakdown Studies: Earlier runs showed a breakdown dependence on pressure. We may explore the limit by lowering the pressure and/or raising the power and trying to pinpoint what breaks down — the input WR650 waveguide, the CTO, or the TE 01 mode in the “big pipe”. To this end, we plan to install acoustic sensors, a TE 01 -sensitive antenna, and perhaps a camera looking in through a hole in the end plate. TE 01 Bend: When the TE bend is fabricated, it can be cold tested using the transmission optimized CTO launchers. For high- power testing, it will be inserted into the KCS waveguide run and transmission and resonant tests will be repeated.

Coming Up Big Long Pipe: We’ve placed an order for ~80 m more KCS main waveguide (WC1890) for a longer installation. While still short compared to runs in an ILC KCS, this will allow us to evaluate longer range transmission. The main motivation for this extension of our experimental setup was to verify that nothing bad happens when more stored energy is available to a breakdown. Resonating this line up to the same field level (300 MW TW-equiv.) will require more power, but we should have enough from our Thales tube with moderate overcoupling to broaden the resonance. … ~80 m

Long KCS Waveguide Support We are building a mezzanine in End Station B at SLAC, running back into the tunnel, to support our extended “big long pipe” experiments.

Recommended CTO Testing and Development: It is important for KCS that we be able to accurately achieve desired CTO couplings. With only two 3dB CTO’s, we cannot directly test their couplings. With both of them employed as matched launchers, we’ll have a test bed into which we can insert other CTO’s to measure their match and extracted power. We should plan to build at least a couple more to do this. We might also try to develop a method to experimentally fine-tune CTO’s as a step in the fabrication process.

300 MW 160 m of WC1890 directional coupler tap-offtap-in phase shifter Future Aspiration KCS Waveguide Resonant Ring: With a resonant ring, we could build up actual rf power levels required in an ILC KCS in a TW mode. This would allow more realistic demonstration and testing of waveguide and components. It would require using our 10MW Toshiba MBK and likely a second klystron. It would also require a 4-port directional coupler capable of driving it in the TE 01 mode and, ideally, a diagnostic directional coupler to measure power level and directionality. One can imagine adding a tap-off/tap-in CTO-based assembly, as shown, to test their functionality and power handling.

U-bend configuration of high-power TE 01 bend for resonant ring ”7.315” 2.045” ” Resonant Ring Turn-Around gaskets

160 m Resonant Ring in ESB