Summary of the test structure design

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

CLIC08 workshop Structure production: CERN activities and Master Schedule G. Riddone, W. Wuensch, R. Zennaro, Contributions from C. Achard, S. Atieh, V.
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,
Choke-mode Damped X-band Structure for CLIC Main Linac Hao ZHA, Jiaru SHI CERN Sep 27, 2011 Jiaru Shi, LCWS11 Workshop, Granada1.
Choke-mode damped accelerating structures for CLIC main linac Hao Zha, Tsinghua University Jiaru Shi, CERN
CLIC drive beam accelerating (DBA) structure Rolf Wegner.
ABSTRACT A damped detuned structure (DDS) for the main linacs of CLIC is being studied as an alternative design to the present baseline heavily damped.
INVESITGATION OF AN ALTERNATE MEANS OF WAKEFIELD SUPPRESSION IN CLIC MAIN LINACS CLIC_DDS.
CARE07, 29 Oct Alexej Grudiev, New CLIC parameters. The new CLIC parameters Alexej Grudiev.
July Alexej Grudiev, Improvement of CLIC structure. Possible improvement of the CLIC accelerating structure. From CLIC_G to CLIC_K Alexej.
CLIC RF structure master schedule and CERN production
INVESITGATION OF AN ALTERNATE MEANS OF WAKEFIELD SUPPRESSION IN CLIC MAIN LINACS CLIC_DDS.
ABSTRACT A damped detuned structure (DDS) for the main linacs of CLIC is being studied as an alternative design to the present baseline heavily damped.
Wakefield suppression in the CLIC main accelerating structures Vasim Khan & Roger Jones.
Design of Standing-Wave Accelerator Structure
Wakefield suppression in the CLIC main accelerating structures Vasim Khan & Roger Jones.
Different mechanisms and scenarios for the local RF
CLIC Drive Beam Linac Rolf Wegner. Outline Introduction: CLIC Drive Beam Concept Drive Beam Modules (modulator, klystron, accelerating structure) Optimisation.
Structure Nick-Names and Documentation Germana creates/created a structure traveler describing the handling (Features: each step, with date and description,
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.
An Overview of the CLIC Testing Program W. Wuensch CLIC ACE
TD24 R05 N1 after high-power test analysis plans A. Degiovanni, M. Aicheler, N. Mouriz Irazabal, A.T. Perez Fontenla, R. Wegner CLIC RF Structure Development.
X-Band RF Structure and Beam Dynamics Workshop, December 2008 CERN experience with 12 GHz high power waveguide components Igor Syratchev (CERN)
Overview of CLIC main linac accelerating structure design 21/10/2010 A.Grudiev (CERN)
2nd CLIC Advisory Committee (CLIC-ACE), CERN January 2008 Introduction to the CLIC Power Extraction and Transfer Structure (PETS) Design. I. Syratchev.
RF structure design KT high-gradient medical project kick-off Alberto Degiovanni TERA Foundation - EPFL.
New RF design of CLIC DB AS Alexej Grudiev, BE-RF.
Overall strategy for the rf structure development program W. Wuensch CLIC ACE
CLIC crab cavity design Praveen Ambattu 24/08/2011.
Recent high-gradient results, rf testing, places and plans Steffen Döbert, CLIC Workshop, Test facilities High gradient results Future testing.
The Zipper Structure: A Novel Accelerator Structure Configuration Christopher Nantista SLAC AAC Workshop ’08 Santa Cruz, CA July 31, 2008.
CLIC Power Extraction and Transfer Structure.
Hybrid designs - directions and potential 1 Alessandro D’Elia, R. M. Jones and V. Khan.
Optimization of CLIC-G structure & Design of CLIC open structure Hao Zha, Alexej Grudiev (CERN) Valery Dolgashev (SLAC) 27/01/2015.
TESLA DAMPING RING RF DEFLECTORS DESIGN F.Marcellini & D. Alesini.
Tolerances coming from RF Alexej Grudiev 24 Nov 2014 X-band accelerating structure review.
Optimization of waveguide geometry in the CLIC-G structures Hao Zha 13/08/2014.
1 Design and objectives of test accelerating structures Riccardo Zennaro.
Accelerating structure prototypes for 2011 (proposal) A.Grudiev 6/07/11.
Feasibility and R&D Needed For A TeV Class HEP e+e- Collider Based on AWA Technology Chunguang Jing for Accelerator R&D Group, HEP Division, ANL Aug
Advancements on RF systems D. Alesini (LNF-INFN) Quinto Meeting Generale Collaborazione LI2FE, Frascati 15-16/03/2011.
Structure Wakefields and Tolerances R. Zennaro. Parameters of the CLIC structure “CLIC G” (from A. Grudiev) StructureCLIC_G Frequency: f [GHz]12 Average.
Status of the sub-harmonic bunching system for the CLIC DB injector front end Hamed Shaker School of Particles and Accelerators, Institute for Research.
Franck PEAUGER – CEA SACLAY LCWS11 - Grenada 29 th September 2011 High power RF components F. Peauger, A. Branco, M. Desmons, W. Farabolini, P. Girardot,
Test Accelerating Structures Designs, Objectives and Critical Issues
Wake-fields simulations and Test Structure
New test structures for CLIC (RF design)
Abstract EuSPARC and EuPRAXIA projects
Vasim Khan & Roger Jones
A 2.3 GHz BANDWIDTH STRUCTURE FOR CLIC_DDS
Status of the CLIC main beam injectors
Optimisation of single bunch linac for FERMI upgrade
RF Power Generation and PETS Design
CLIC_DDS study
Design Fabrication and Processing Group H. Padamsee
EM characterization of SiC
Application of the moderate peak power (6 MW) X-band klystron’s cluster for the CLIC accelerating structures testing program. I. Syratchev.
Review of rf structure test results
Testing Infrastructure, Program and Milestones
Tolerances: Origins, Requirements, Status and Feasibility
F.Marcellini, D.Alesini, A.Ghigo
Update of CLIC accelerating structure design
Status of the CLIC Injector studies
Progress in the design of a damped an
Accelerator Physics Particle Acceleration
CLIC Power Extraction and Transfer structure (PETS)
TCLIA/TCTV transverse BB impedance versus gap size
TCLIA/TCTV transverse BB impedance versus gap size
Presentation transcript:

Summary of the test structure design Grudiev 14/04/2010

11.424 GHz, <100 MV/m>, 100 ns, reg. cells CLIC_vg1: undamped damped edms#1065638 edms#1065641 edms#1065642 50% 41% 47% CLIC_G: undamped damped edms#1065640 edms#1065643 edms#1065646 18% 8% 13% A. Grudiev, 14/04/2010

11.994 GHz, <100 MV/m>, 100 ns, reg. cells CLIC_G: undamped damped edms#1068314 edms#1070498 edms#1069239 17% 8% 8% new A. Grudiev, 14/04/2010

Preliminary Design of the Damping Load Will be used for CLIC module prototype and for a structure prototype for high power testing with damping load inside (TD24_vg1.8_diskR05_SiC) SiC properties from M.Luong, 1999 thick line: awg = 11mm, thin line: awg = 10.1 mm Tip size 1x1 mm Tip length 20 mm or 30 mm Base size 5.6 x 5 or 5.5 mm Base length 10 mm Waveguide width awd = 10.1 mm or 11 mm A. Grudiev, 14/04/2010

Design of the damped compact coupler Will be used for CLIC module prototype and for a structure prototype for high power testing with damped compact coupler (TD26_vg1.8_diskR05_CC) A. Grudiev, 14/04/2010

Beyond CLIC_G A structure with a degree of tapering lower than TD18_vg2.6_disk (41%) and TD24_vg1.8_diskR05 (8%) is an interesting option For example, ~ 20-25 % It could also have bigger average aperture if CLIC main beam bunch charge can be increased accordingly. A detailed optimization of the parameters and rf design will be done this year A. Grudiev, 14/04/2010

The test matrix (all structures in disks) R. Zennaro 2008 In red: 11.4 GHz new structures (C10) In blue: 30 GHz new structures (scaled values for a and d) (C30) d [mm] a [mm] 2.79 2.13 2.00 1.66 1.37 1.25 2.53 Vg: 0.7% CLIC _vg1 output 1.0% 2.85 T53 output 1.0% 3.0 CERN-X 1.1% Vg: 1.35% 3.87 3.89* Vg: 2.25% (*) 30 GHz 2π/3 ≈2.6% T53 input Vg: 3.3% 4.38 30 GHz 2π/3 4.7% 5.00 30 GHz π/2 7.4% 2π/3 8.2% Direct comparison of variation of a and P/c Direct comparison of variation of d Damped version? Direct comparison of variation of P/c Test for a relatively large group velocity KEK 005/13/2008 (*) not very different from input vg1 (d=2.79; a=4.06)

C10 family Aperture scan (un-damped cells) C10_vg1.35 C10_vg0.7 Different damping geometry (damped cells with iris geometry from C10_vg1.35) CD10_WDS different materials are on hold CD10_Choke (edms#1071742) different choke gap will be investigated C10 family is still a valid approach because it is simpler and cheaper than a full scale tapered structure prototype. The main problem is lower priority so it goes very slow, much slower than tapered structures. (C10-paradox !) A. Grudiev, 14/04/2010

Single-feed mode launcher Design for C10 structures E-field H-field -40dB BW 90 MHz A. Grudiev, 14/04/2010

Quadrants/halves family Here T18_vg2.6_quad design is used. It has no slots. QUADs with SLOTS T18_vg2.6_Qslot design is used. It is the T18_vg2.6_quad but 4 slots of 0.2 mm rounded with 0.2mm radius are introduced. Corresponding frequency up-shift is ~1 MHz, well within tuning range. A. Grudiev, 14/04/2010