Structures design R&D program Alessandro D’Elia-UMAN/CI and CERN On behalf of Roger M. Jones 1.

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Presentation transcript:

Structures design R&D program Alessandro D’Elia-UMAN/CI and CERN On behalf of Roger M. Jones 1

2  Roger M. Jones (Univ. of Manchester faculty)  Alessandro D’Elia (Dec 2008, Univ. of Manchester PDRA based at CERN)  Vasim Khan (PhD student, Sept 2007)  Nick Shipman (PhD student Sept 2010, largely focused on breakdown studies)  Part of EuCARD ( European Coordination for Accelerator Research and Development) FP7 NCLinac Task 9.2  Major Collaborators: W. Wuensch, A. Grudiev, I. Syrachev, R. Zennaro, G. Riddone (CERN) Wake Function Suppression for CLIC-Staff V. Khan, CI/Univ. of Manchester Ph.D. student graduated April 2011 (now CERN Fellow) A. D’Elia, CI/Univ. of Manchester PDRA based at CERN (former CERN Fellow). N. Shipman, CERN/CI/Univ. of Manchester Ph.D. student R. M. Jones, CI/Univ. of Manchester, Accelerator Group Leader

A Detuning Damping Structure (DDS) for CLIC 3 The present CLIC structure relies on linear tapering of cell parameters and heavy damping with a Q of ~10. Wake function suppression entails heavy damping through waveguides and dielectric damping materials in relatively close proximity to accelerating cells. Choke mode suppression provides an alternative, but may negatively impact R sh A viable alternative is presented by CLIC_DDS design - parallels the DDS developed for the GLC/NLC- and entails: 1. Detuning the dipole bands by forcing the cell parameters to have a precise spread in the frequencies -presently Gaussian Kdn/df- and interleaving the frequencies of adjacent structures. 2. Moderate damping Q ~

CLIC_DDS_A 4 In October 2009 it has been decided to produce a first prototype to be tested at input power of 62 MW to ascertain the suitability of the structure to sustain high e.m. field gradients RF and mechanical design completed in Summer qualification disks machined by VDL received in Oct 2010 The 4 disks have been successfully bonded by Bodycote The whole structure will be machined in Japan by Morikawa under the supervision of KEK High Power Tests are foreseen as soon as we will get the full structure NOW

CLIC_DDS_B The study of a further structure (CLIC_DDS_B) is already started This structure will be based on CLIC_DDS_A but will be provided with HOM couplers and with Compact Fundamental coupler Both wakefield suppression and high power performances will be tested Next future 5

CLIC_DDS_A: regular cell optimization The chose of the cell geometry is crucial to meet at the same time: 1.Wakefield suppression 2.Surface fields in the specs Consequences on wake function Cell shape optimization for fields DDS1_CDDS2_E 6

Further information: Manifold dimensions are uniform throughout the structure The manifold radius is now parameterised in order to keep the lowest manifold mode above 12 GHz. CLIC_DDS_A: regular cells, final design Roundings enhance the magnetic field however a reduction of the slot size mitigates this enhancement and RF parameters are back within required limits. Also the wake damping is still in the limits with margins for a further improvement. 7

CLIC_DDS_A full structure 8

CLIC_DDS_A some further detail VDL BODYCOTE 9

First steps toward CLIC_DDS_B Wakefield calculations for DDS are, in the early design stage, based on single infinitely periodic cells. Though cell-to-cell interaction is taken into account to calculate the wakefields, it is important to study full structure properties using computational tools. GdfidL impedance 10

Recalculation of Kicks and Q’s from the impedance Lorentzian fit of the peaks Qdip Kick factor Peak 1 Procedure 11

Preliminary HOM coupler thoughts Same technique as for matching cells No common minima 18GHz 12

Standard DDS Manifold Additional Manifold 13 I/P at  /2  =15.9GHz Work in Progress/R&D Opportunities  CLIC_DDS_A is equipped with mode launchers  CLIC_DDS_B includes full HOM ports  Initial studies on matching the HOM coupler for CLIC_DDS_B in progress (dipole band ~ 15.9 GHz – 18 GHz) Sic  Moving to a high phase advance (HPA) structure allows other parameters to be optimised  5  /6 phase advance structure design in progress (for initial design see Linac2010)  In the HPA design further features being explored  Additional manifold (8)  Influence of SiC rods on overall Q Enhanced Coupling

14  CLIC_DDS_A : RF (including mode launcher matching cells) and mechanical design has been completed.  Qualifications cells fabricated (VDL)–all cells by last quarter 2010  Structure will be subsequently bonded in the first quarter of 2011, -- ready for high power testing in 2011 at the CLIC test stand.  CLIC_DDS_B: Includes HOM couplers and power coupler. HOM coupler design in progress. Final Remarks  Transfer cell fabrication to Morikawa in collaboration with KEK  Cell ETA April qualification cells, followed by full 24 cells  Recent events in Japan have affected schedule –full structure expected during last quarter of 2011  RF cold test measurements (S21) at KEK  New CLIC_DDS R&D in progress:  HPA: High phase advance design is being studied. It Allows optimisation of the remaining parameters –minimise surface fields, wakefields at stipulated v g  Further optimisation is being explored by implementing additional manifolds and with the potential for the insertion of SiC rods to reduce the Q further

15  I am pleased to acknowledge a strong and fruitful collaboration between many colleagues and in particular, from those at CERN, University of Manchester, Cockcroft Inst., SLAC and KEK.  Several at CERN and KEK within the CLIC programme, have made critical contributions: W. Wuensch, A. Grudiev, I. Syrachev, R. Zennaro, G. Riddone (CERN), T. Higo Y. Higashi (KEK). Acknowledgements 1.R. M. Jones, et. al, PRST-AB, 9, , V. F. Khan and R.M. Jones, EPAC08, V. F. Khan and R.M. Jones, LINAC08, V. F. Khan and R.M. Jones, Proceedings of XB08, R. M. Jones, PRST-AB, 12, , R. M. Jones, et. al, NJP, 11, , V. F. Khan and R.M. Jones, PAC09, V. F. Khan, et. al, IPAC10, V. F. Khan, et. al, LINAC10, CLIC DDS Related Pubs.

Thanks 16