Dual mode 5-9-12 6 bph 30 bph TMF TMR TMF TMR TEF TER.

Slides:



Advertisements
Similar presentations
Dual mode bph6 bph TM F TM R TE R TE F TM F TM R.
Advertisements

Breakdown Rate Dependence on Gradient and Pulse Heating in Single Cell Cavities and TD18 Faya Wang, Chris Nantista and Chris Adolphsen May 1, 2010.
Single-Cell Standing Wave Structures: Design
CLIC08 workshop Structure production: CERN activities and Master Schedule G. Riddone, W. Wuensch, R. Zennaro, Contributions from C. Achard, S. Atieh, V.
Single cell standing wave tests data analysis Jiaru Shi Sep 27, 2011 LCWS11, Granada, Spain.
CLIC drive beam accelerating (DBA) structure Rolf Wegner.
Development of an X-band Dielectric PETS C. Jing, Euclid Techlabs / ANL HG Workshop, May
Report from KEK High gradient study results from Nextef (+ other related activities) LCWS2011, Granada Sep. 27, 2011 T. Higo.
X-band Structures Test Results at NLCTA Faya Wang Chris Adolphsen, Christopher Nantista 9-Feb-11.
Injector RF Design Review November 3, 2004 John Schmerge, SLAC  and 0 Mode Interaction in RF Gun John Schmerge, SLAC November.
Injector RF Design Review November 3, 2004 John Schmerge, SLAC LCLS RF Gun Thermal Analysis John Schmerge, SLAC November 3,
1 X-band Single Cell and T18_SLAC_2 Test Results at NLCTA Faya Wang Chris Adolphsen Jul
AC Power Supplies Applications –Standby source for “critical” loads (computer) –Primary source when normal ac not available Uninterrupted Power Supply.
Dual Mode Cavity for Testing Effects of RF Magnetic field on Breakdown Properties A. Dian Yeremian, Valery Dolgashev, Sami Tantawi SLAC National Accelerator.
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.
Alessandro Cappelletti for CTF3 collaboration 5 th May 2010 RESULTS OF BEAM BASED RF POWER PRODUCTION IN CTF3.
High power RF capabilities From Two 50 MW Klystrons Variable iris Variable Delay line length through variable mode converter Gate Valves Two experimental.
Test Facilities Sami Tantawi SLAC. Summary of SLAC Facilities NLCTA (3 RF stations, one Injector, one Radiation shielding) – Two 240ns pulse compressor,
HIGH RF POWER TESTING FOR THE CLIC PETS International Workshop on Linear Colliders 20 th October 2010 Alessandro Cappelletti for the CLIC team with.
Photonic Band Gap Accelerator Experiments Roark Marsh Massachusetts Institute of Technology, Plasma Science and Fusion Center Accelerator Seminar 1/27/2009.
Particle-in-Cell Modeling of Rf Breakdown in Accelerating Structures and Waveguides Valery Dolgashev, SLAC National Accelerator Laboratory Breakdown physics.
PULSE SHAPING ISSUES FOR THE PETS TESTING PROGRAM AT SLAC A.Cappelletti SLAC, Oct 2008.
Development of Dielectric-Based Wakefield Power Extractors Chunguang Jing 1,2, W. Gai 1, A. Kanareykin 2, Igor Syratchev, CERN 1. High Energy Physics Division,
Test Facilities and Component Developments Sami Tantawi SLAC May 15, 2008.
1 C-Band Linac Development Satoshi Ohsawa 2004.Feb.19LCPAC.
10th ITPA conference, Avila, 7-10 Jan Effects of High Energy Ions Accelerated in front of ICRF Antennas in LHD S. Masuzaki on behalf of the LHD Experimental.
June 2007, CERN. HDS 60 (cells) copper was processed from both sides Low Vg a/λ=0.16 High Vg a/λ=0.19 HDS 11 titanium Very often we do observe, that after.
PEP-II Machine Advisory Committee Meeting SLAC, April 15-17, 2004 HOM Issues in LER Ring and IR. Recent measurements and calculations. Sasha Novokhatski.
Development of Dielectric PETS Chunguang Jing and Wei Gai ANL and Euclid CLIC workshop 2013.
NLC Status and Milestones D. L. Burke ISG9 KEK December 10-13, 2002.
L-band (1.3 GHz) 5-Cell SW Cavity High Power Test Results Faya Wang, Chris Adolphsen SLAC National Accelerator Laboratory
Frequency-domain study of acceleration & beam loading based on a circuit model by raquel fandos.
Next Linear Collider 8-Pack Project D. Atkinson System Review, April 3 The 8-Pack Project at NLCTA An overview of the status and schedule for the project.
PBG Structure Experiments, AAC 2008 Photonic Bandgap Accelerator Experiments Roark A. Marsh, Michael A. Shapiro, Richard J. Temkin Massachusetts Institute.
Measurements of the X-ray/pump laser pulse timing Valery Dolgashev, David Fritz, Yiping Feng, Gordon Bowden SLAC 48th ICFA Advanced Beam Dynamics Workshop.
KEK workshopWalter Wuensch18 April 2012 Status and objectives of the CLIC X-band and high- gradient activity.
PETS TESTING ANALYSIS 4 th X-band Structure Collaboration Meeting 3 rd May 2010 Alessandro Cappelletti for CLIC collaboration.
KCS and RDR 10 Hz Operation Chris Adolphsen BAW2, SLAC 1/20/2011.
Some Results and Analysis from CTF3 1HG2012-April-18 Some Results and Analysis from CTF3 W. Farabolini - A. Palaia.
GHz High Gradient Testing of a T18 TW StructureUsing a Fast Response Protection and Power Recirculating System GHz High Gradient Testing.
Review of the rf working group of the ICFA Mini Workshop on Novel Accelerators and Colliders which was associated with the Bob Siemann Memorial Symposium.
I. Syratchev, structure team meeting, Re-circulation Re-visited I. Syratchev.
HLRF R&D Towards the TDR Christopher Nantista ML-SCRF Webex meeting June 29, 2011.
The US High Gradient Collaboration Vision for Research and Development on Ultra High Gradient Accelerator Structures Sami Tantawi, SLAC ( on behalf of.
June 16, 2015 CLIC WORKSHOP JANUARY 18 – 22, 2016 OPTIMIZED RF UNIT I 1 January 21, 2016 By: Mikael Lindholm.
Update on SLAC experiments with High Gradient Accelerators and RF Components M.Franzi, V.A. Dolgashev, S. Tantawi June 6, 2016.
Superconducting Materials Testing With a High-Q Copper RF Cavity Sami Tantawi, Valery Dolgashev, Gordon Bowden, James Lewandowski, Christopher Nantista.
2010 TESTING PROGRAM AND RESULTS FOR THE CLIC PETS X-BAND WORKSHOP ON RF STRUCTURES, BEAM DYNAMICS AND SOURCES 2 nd December 2010 Alessandro Cappelletti.
Advancements on RF systems D. Alesini (LNF-INFN) Quinto Meeting Generale Collaborazione LI2FE, Frascati 15-16/03/2011.
A CW Linac scheme for CLIC drive beam acceleration. Hao Zha, Alexej Grudiev 07/06/2016.
RF Pulse Compression system for CTF3.
Test Accelerating Structures Designs, Objectives and Critical Issues
Multi-stage pulse compressor
A 6 GeV Compact X-ray FEL (CXFEL) Driven by an X-Band Linac
Breakdown position analysis
Development of X-band 50MW klystron in BVERI
SLAC National Accelerator Laboratory
Physics design on Injector-1 RFQ
Brief Review of Microwave Dielectric Accelerators
Review of rf structure test results
Recent high-gradient testing results from the CLIC XBoxes
Status of T18 in resonant ring processing
Progress in the design of a damped an
RF Pulse Shaping.
5th X-Band Structure Collaboration Meeting
T18_VG2.4_Disk_#2 processing summary
A proposal for a pulsed surface heating experiment in a CLIC accelerating structure using variable pulse length Alexej Grudiev.
CEPC SRF Parameters (100 km Main Ring)
Field-Emission mapping measurement on Copper Surface
Presentation transcript:

Dual mode 5-9-12 6 bph 30 bph TMF TMR TMF TMR TEF TER

ASTA now T18 processing without ring Valery Dolgashev, Jim Lewandowski and Stephen Weathersby 1 June 2011 SLAC

T18 sans ring installed. This requires twice the input power to maintain the same gradient as the ring configuration. This test will elucidate the effect of the ring (previous test) on structure performance.

88 MW @ Frequency 1. 142440E+10, 200 ns pulsewidth 88 MW @ Frequency 1.142440E+10, 200 ns pulsewidth. Vacuum activity mainly on the input side of the structure. 13 breakdowns at this level.

Status of T18 in resonant ring processing Valery Dolgashev, Jim Lewandowski and Stephen Weathersby 13 April 2011 SLAC

Two rings couple the input and output power of the T18 (18 cells) travelling wave accelerator structure. Reduces the required input power and hopefully enhances the performance of the structure. Also, the ring configuration is thought to reduce the damaging effects of breakdowns by distributing the breakdown power over time.

Pulse shape, 100 ns charging + 1500 ns flat structure input ring load structure input ring input pulse heating File: ppm_data_Mar29_2011, trace#: 1200 with time stamp:{29,3,2011,10,29,51,210} PulseLength:1.54 [us] Pulse Heating: 8.63429 [deg. C]

Pulse shape, 100 ns charging + 600 ns flat structure input structure input ring load ring input pulse heating File: ppm_data_Apr05_2011 , trace#: 1200 with time stamp: {5,4,2011,8,39,44,128} PulseLength: 0.64 [us] Pulse Heating: 34.037 [deg. C]

Pulse shape, 100 ns charging + 250 ns flat structure input structure input ring input pulse heating ring load File: ppm_data_Apr12_2011, trace#: 1200 with time stamp:{12,4,2011,8,41,20,757} Max. PulseLength:0.28 [us] Pulse Heating: 24.885 [deg. C]

Pulse shape, 100 ns charging + 100 ns flat structure input structure input ring input pulse heating ring load File: ppm_data_Apr20_2011 , trace#: 1200 with time stamp: {20,4,2011,8,22,35,155} PulseLength: 0.12 [us] Pulse Heating: 18.169 [deg. C]

T18 in resonant ring, last ~180 hours of processing up to end of shift on April 21st 2011 100 ns flat 250 ns flat 1.5 us flat 600 ns flat 100 ns flat 250 ns flat 1.5 us flat 600 ns flat 1.5 us flat 600 ns flat 250 ns flat 100 ns flat

Summary of T18 in resonant ring up to end of shift on April 12th 2011 250 ns 400 ns 200 ns 200 ns 1500 ns 250 ns 100 ns 1500 ns 100 ns 600 ns 600 ns 400 ns Valery Dolgashev, Jim Lewandowski and Stephen Weathersby, 13 April 2011

Summary of T18 in resonant ring up to end of shift on April 21st 2011 250 ns 400 ns 200 ns 200 ns 1500 ns 250 ns 100 ns 1500 ns 100 ns 600 ns 600 ns 400 ns 100 ns (2nd experiment) 100 ns (2nd experiment) Valery Dolgashev, Jim Lewandowski and Stephen Weathersby, 26 April 2011