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.

Slides:



Advertisements
Similar presentations
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.
Advertisements

COOLING TUBE ACCELERATING STRUCTURE MANIFOLD COUPLER VACUUM INTERFACE FLANGE RF INTERFACE FLANGE TUNING STUD ENGINEERING DESIGN AND FABRICATION OF X-BAND.
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.
Compact Linear Collider. Overview The aim of the CLIC study is to investigate the feasibility of a high luminosity linear e-/e+ collider with a centre.
ABSTRACT We report on the suppression of long-range wakefields in the main linacs of the CLIC collider. This structure operates with 2π/3 phase advance.
R.M. Jones, International Workshop on Linear Colliders, 18 – 22 Oct. 2010, CERN, Geneva 1 Status and Prospects for the CLIC DDS Roger M. Jones Cockcroft.
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.
4th CLIC Advisory Committee (CLIC-ACE), 26 th - 28 th May Alternate Means of Wakefield Suppression in CLIC Main Linac Roger M. Jones, Vasim Khan,
MAIN LINAC DDS DESIGN Vasim Khan Bohr seminar series, HEP group, The University of Manchester.
INVESITGATION OF AN ALTERNATE MEANS OF WAKEFIELD SUPPRESSION IN CLIC MAIN LINACS CLIC_DDS.
A 2.3 GHz BANDWIDTH STRUCTURE FOR CLIC_DDS Vasim Khan
International Workshop on Linear Colliders, 18 – 22 Oct. 2010, CERN, Switzerland 1 Recent progress on CLIC_DDS Roger M. Jones Cockcroft Institute and The.
Vasim Khan 4th Annual X-band Structure Collaboration Meeting, CERN /36 CLIC_DDS & Test Structure V. Khan, A. D’Elia, R. Jones A.
CLIC MAIN LINAC DDS Vasim Khan. 24 cells No interleaving 48cells 2-fold interleaving ∆fmin = 32.5 MHz ∆tmax =30.76 ns ∆s = 9.22 m 24 cells No interleaving.
ABSTRACT The main accelerating structures for the CLIC are designed to operate at 100 MV/m accelerating gradient. The accelerating frequency has been optimised.
Vasim Khan X-Band RF Structures, Beam Dynamics and Sources Workshop, Cockcroft Institute /13 CLIC_DDS study
CLIC MAIN LINAC DDS DESIGN AND FORTCOMING Vasim Khan & Roger Jones V. Khan LC-ABD 09, Cockcroft Institute /14.
Wakefield suppression in the CLIC main accelerating structures Vasim Khan & Roger Jones.
Design of Standing-Wave Accelerator Structure
Vasim Khan X-Band RF Structures, Beam Dynamics and Sources Workshop, Cockcroft Institute /21 CLIC_DDS_HPA study
Wakefield suppression in the CLIC main accelerating structures Vasim Khan & Roger Jones.
Vasim Khan X-Band RF Structures, Beam Dynamics and Sources Workshop, Cockcroft Institute /24 CLIC_DDS study
WAKEFIELD SUPPRESSION IN THE MAIN LINACS OF CLIC Vasim Khan The Cockcroft Institute of Accelerator Science and Technology, Daresbury, Warrington, WA4 4AD.
ABSTRACT The main accelerating structures for the CLIC are designed to operate at 100 MV/m accelerating gradient. The accelerating frequency has been optimised.
DDS limits and perspectives Alessandro D’Elia on behalf of UMAN Collaboration 1.
CLIC Drive Beam Linac Rolf Wegner. Outline Introduction: CLIC Drive Beam Concept Drive Beam Modules (modulator, klystron, accelerating structure) Optimisation.
INTEGRATION OF RF STRUCTURES IN THE TWO-BEAM MODULE DESIGN G. Riddone, CERN, Geneva, Switzerland A. Samoshkin, D. Gudkov, JINR, Dubna, Russia Abstract.
Course B: rf technology Normal conducting rf Part 5: Higher-order-mode damping Walter Wuensch, CERN Sixth International Accelerator School for Linear Colliders.
Structures design R&D program Alessandro D’Elia-UMAN/CI and CERN On behalf of Roger M. Jones 1.
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.
SRF CAVITY GEOMETRY OPTIMIZATION FOR THE ILC WITH MINIMIZED SURFACE E.M. FIELDS AND SUPERIOR BANDWIDTH The Cockcroft Institute of Accelerator Science and.
ABSTRACT The Compact Linear Collider (CLIC) is currently under development at CERN as a potential multi-TeV e + e – collider. The manufacturing and assembly.
ENGINEERING DESIGN AND FABRICATION OF X-BAND DAMPED DETUNED STRUCTURE V. Soldatov¹, D. Gudkov¹, A. Samoshkin¹, G. Riddone², A. Grudiev², S. Atieh², A.
R.M. Jones, XB Structures Collaboration Workshop, SLAC, 16 th – 18 th May Status of Detuned and Manifold-Damped HG Linacs for CLIC Roger M. Jones.
R.M. Jones, EuCARD2, CERN, 20 th April Detuned and Manifold-Damped HG Linacs for CLIC Roger M. Jones Cockcroft Institute and The University of Manchester.
The CLIC accelerating structure development program Walter Wuensch CARE05 23 November 2005.
MP - HIPPI General meeting, Abingdon October 28-30, Side Coupled Linac Design at CERN Side Coupled Linac Design at CERN M. Pasini, Abingdon September.
ENGINEERING DESIGN AND FABRICATION OF X-BAND ACCELERATING STRUCTURE TD24 WITH WFM Abstract To achieve high luminosity in CLIC, the accelerating structures.
WP 9.2 DDS Status, R.M. Jones, 25 th Oct 2010, WebEx Phone-in, Geneva 1 WP 9.2: DDS Status Roger M. Jones Cockcroft Institute and The University of Manchester.
Hybrid designs - directions and potential 1 Alessandro D’Elia, R. M. Jones and V. Khan.
TWO-BEAM, MULTI-MODE, DETUNED ACCSELERATING STRUCTURE S.Kazakov 1,2, S.Kuzikov 3, V.Yakovlev 4 J.L. Hirshfield 1,5, 1 Omega-p,Inc., 199 Whitney Ave., New.
Optimization of CLIC-G structure & Design of CLIC open structure Hao Zha, Alexej Grudiev (CERN) Valery Dolgashev (SLAC) 27/01/2015.
1 Design and objectives of test accelerating structures Riccardo Zennaro.
Accelerating structure prototypes for 2011 (proposal) A.Grudiev 6/07/11.
XB-10, ICFA Mini-Workshop, R.M. Jones, Cockcroft Inst., 30 th Nov-3 rd Dec Wakefields in Linacs Subjected to Detuning and Manifold Coupled Damping.
Damped and Detuned Structures for CLIC The University of Manchester The Cockcroft Institute 4/10/2013I.Nesmiyan1 Acknowledgements to colleagues at CERN,
A. D’Elia 1,2,3, T. Higo 4, V. F. Khan, R.M. Jones 1,2, A. Latina 3, I. Nesmiyan 1,2, G. Riddone 3 1 School of Physics and Astronomy, The University of.
Damping intense wake-fields in the main Linacs and PETS structures of the CLIC Linear Collider Vasim Khan: 1 st year PhD Student Supervisor: Dr. Roger.
GOLD- ELECTROPLATING COOLING FITTING ADAPTER ACCELERATING STRUCTURE CONCEPTUAL DESIGN OF X-BAND ACCELERATING STRUCTURE TD26 CC SIC Abstract Many accelerating.
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.
Alternate Means of Wakefield Suppression in CLIC Main Linac
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
Roger M. Jones Cockcroft Institute and The University of Manchester
CLIC_DDS study
Developments on Proposed
Summary of the test structure design
Update of CLIC accelerating structure design
CEPC Main Ring Cavity Design with HOM Couplers
Progress in the design of a damped an
CLIC Power Extraction and Transfer structure (PETS)
Presentation transcript:

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 structure (CLIC_G). In our earlier designs [1-2] we studied a detuned structure, operating at GHz, with a range of dipole bandwidths in order to ensure the structure satisfies beam dynamics and rf breakdown constraints [3]. Here we report on the development of a damped and detuned structure which satisfies both constraints. Preparations for high power testing of the structure are also discussed. International Particle accelerator conference, IPAC’10, May 23 – 28, Kyoto, Japan. STRUCTURE WITH RELAXED PARAMETERS: CLIC_DDS_C Modifying the bunch spacing to 8 rf cycles (~0.67 ns) allowed the transverse wakefield to be damped sufficiently once the structure is provided with a bandwidth of ~ 2.3 GHz. The dipole frequencies of 24 cells are detuned by employing an erf (error) function variation of each iris with cell number. The recoherence in the wakefield is prevented by coupling it out through slots in each cell to the attached manifolds. This adversely affects the magnetic field and gives rise to an unacceptable surface pulse temperature rise (∆T). RECENT PROGRESS ON A MANIFOLD DAMPED AND DETUNED SRUCTURE FOR CLIC V. F. Khan †*, A. D’Elia †*‡, A. Grudiev ‡, R. M. Jones †*, W. Wuensch ‡, R. Zennaro ‡ † School of Physics and Astronomy, The University of Manchester, Manchester, U.K. * The Cockcroft Institute of Accelerator Science and Technology, Daresbury, U.K. ‡ CERN, Geneva, Switzerland. CLIC_DDS_C SPECIFICATIONS Twenty four cells per structure Eight structures interleaved Dipole bandwidth, ∆f = 3.3 GHz =3.6 σ Detuning : 13.7 % of central frequency Taper in iris : 4 mm to 2.3 mm Excellent wakefield suppression Unacceptable rise in surface fields due to coupling slots. ELLIPTICAL WALL : CLIC_DDS_E Modifying the surface of the outer wall succeeds in reducing monopole H-field and ∆T. This reduces the dipole e.m. field in the vicinity of the slots and hence reduces the efficacy of manifold damping. Mechanical engineering considerations (rounding of edges and corners) exacerbates the reduction in coupling. Nonetheless, the wakefield is still more than adequately suppressed! H-FIELD OPTIMISATION In order to redistribute the field in the region of the slot-coupeld manifold we considered various elliptical wall geometries. Both convex and concave were considered. Final optimised shape reduces ∆T by ~ 23% (65 0 K to 51 0 K). Cell 1 Cell 24 Cell1 Cell24 H-field 40 0 K 51 0 K Sc [6]: Modified Poynting vector 6.75 W/μm 2 E-field 220 MV/m Cell 1 Cell 24 ACKNOWLEDGEMENTS V. Khan acknowledges receipt of funding from the Cockctoft Institute. This research has received funding from the European Commission under FP7 Research Infrastructure grant agreement no Rectangular ε = ∞ Circular ε = 1 Elliptical a b ε = 1.2 ε = ∞ ε = 0.8 ε = 1 H-field on a manifold damped single cell wall ε = 1.2 Elliptical shape CLIC_DDS_A : RF properties CLIC_DDS_A : Envelope of wakefield in a single structure CLIC_DDS_A : RF params.UnitValues Fundamental mode Q (In / Out)-5020 / 6534 Shunt impedance R’ (In / Out)MΩ/m51 / 118 Group velocity (In / Out)%2.07 / 1.0 Bunch population (N b )-4.2 x 10 9 Peak input power (P in) MW71 Pulse length (Total/ flat top)ns277 / 208 Acc. grad. (Load./Unload.)MV/m105 / 132 Pulsed temp. rise ( ) oKoK51 Surface electric field ( )MV/m220 Modified Poynting vector ( )W/μm RF-beam efficiency (η)%23.5 HIGH POWER TEST : CLIC_DDS_A RF design complete, mechanical design in progress! A single structure will be tested at input power of 71 MW/m to ascertain the suitability of the structure to sustain high e.m. field gradients. Surface fields are within acceptable limits! Structure fabrication and tests by the first quarter of 2011! WEPE032 CLIC_DDS_C : Spectral function(G) CLIC_DDS_C : Envelope of wakefield in an 8-fold interleaved structure Kdn/df [4-5] G [4-5] CLIC_DDS_E : Spectral function(G) CLIC_DDS_E : Envelope of wakefield in an 8-fold interleaved structure Kdn/df [4-5] G [4-5] Lowest dipole mode Manifold Manifold coupling slot REFERNCES [1] V.F. Khan and R.M. Jones, EPAC08, [2] V.F. Khan and R.M. Jones, LINAC08, [3] H. Braun, et. al, CLIC-Note764, [4] R.M. Jones, et. al, PRST-AB, 9, , [5] R.M. Jones, et. al, NJP, , [6] A. Grudiev, et. al, PRST-AB, , DS Q cu ~ 5930 CLIC_DDS_A DS Q cu ~ 5860 CLIC_DDS_E Beam dynamics constraint Recoherence position DS Q cu ~ 5780 CLIC_DDS_C Beam dynamics constraint Recoherence position