Tolerances: Origins, Requirements, Status and Feasibility

Slides:



Advertisements
Similar presentations
CLIC08 workshop Structure production: CERN activities and Master Schedule G. Riddone, W. Wuensch, R. Zennaro, Contributions from C. Achard, S. Atieh, V.
Advertisements

PETS components and waveguide connections CLIC Workshop 2007 David Carrillo.
Emittance dilution due to misalignment of quads and cavities of ILC main linac revised K.Kubo For beam energy 250 GeV,
Emittance dilution due to misalignment of quads and cavities of ILC main linac K.Kubo For beam energy 250 GeV, TESLA-type optics for 24MV/m.
On Cavity Tilt + Gradient Change (Beam Dynamics) K. Kubo K. Kubo.
Probe beam distortion in TBTS due to high gradient RF acceleration (first part: observations) CTF3/TBTS Logbook 17 May 2013 Wilfrid Farabolini – Alexej.
18/6/2007 M.Taborelli, TS-MME Structure fabrication techniques and possibilities M.Taborelli Disk structures Quadrant structures ….most of it inspired.
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.
ABSTRACT The main accelerating structures for the CLIC are designed to operate at 100 MV/m accelerating gradient. The accelerating frequency has been optimised.
A U.S. Department of Energy Office of Science Laboratory Operated by The University of Chicago Argonne National Laboratory Office of Science U.S. Department.
2 nd collaboration meeting on X-band Accelerator Structure Design and Test-Program Structure fabrication Comparative analysis of disk and quadrant manufacture.
Compensation of Transient Beam-Loading in CLIC Main Linac
Status of vacuum & interconnections of the CLIC main linac modules C. Garion TE/VSC TBMWG, 9 th November 2009.
SRF Results and Requirements Internal MLC Review Matthias Liepe1.
International Workshop on Linear Colliders 2010 Design and fabrication update on PSI/Trieste X-band phase- space rotator structure Dmitry Gudkov 21-OCT-2010.
Drive Beam Linac Stability Issues Avni AKSOY Ankara University.
For Draft List of Standard Errors Beam Dynamics, Simulations Group (Summarized by Kiyoshi Kubo)
Particle dynamics in electron FFAG Shinji Machida KEK FFAG04, October 13-16, 2004.
2nd CLIC Advisory Committee (CLIC-ACE), CERN January 2008 Introduction to the CLIC Power Extraction and Transfer Structure (PETS) Design. I. Syratchev.
New RF design of CLIC DB AS Alexej Grudiev, BE-RF.
H.H. Braun, Structure WG, Permissible Trip Rates for 12 GHz structures in CLIC  Type of break downs  Permissible rate for type I RF breakdown.
CLIC08 workshop CLIC module layout and main requirements G. Riddone, on behalf of the CMWG Home page of the TBM WG:
CLIC Workshop th -17 th October 2008 Thomas Zickler AT/MCS/MNC 1 CLIC Main Linac Quadrupoles Preliminary design of a quadrupole for the stabilization.
Beam breakup and emittance growth in CLIC drive beam TW buncher Hamed Shaker School of Particles and Accelerators, IPM.
KEK workshopWalter Wuensch18 April 2012 Status and objectives of the CLIC X-band and high- gradient activity.
5/7/2007 TS_CLIC_AB M.Taborelli, TS-MME High precision machining and metrology for structures: achievements and open questions M.Taborelli.
1 EMMA Tracking Studies Shinji Machida ASTeC/CCLRC/RAL 4 January, ffag/machida_ ppt & pdf.
Beam Dynamics WG K. Kubo, N. Solyak, D. Schulte. Presentations –N. Solyak Coupler kick simulations update –N. Solyak CLIC BPM –A. Latina: Update on the.
10/2007 M.Taborelli, TS-MME M.Taborelli Structure fabrication: dimensional tolerances Contributions of : G.Arnau-Izquierdo, A.Cherif, D.Glaude, R.Leuxe,
ENGINEERING DESIGN AND FABRICATION OF X-BAND ACCELERATING STRUCTURE TD24 WITH WFM Abstract To achieve high luminosity in CLIC, the accelerating structures.
CLIC Stabilisation Day’08 18 th March 2008 Thomas Zickler AT/MCS/MNC/tz 1 CLIC Quadrupoles Th. Zickler CERN.
CLIC accelerating structures: study of the tolerances and short range wakefield considerations R. Zennaro CERN.
Peak temperature rise specification for accelerating structures: a review and discussion CLIC meeting
CLIC workshop ”Two beam hardware and integration” working group Module layout and main requirement G. Riddone, A. Samoshkin
Risto Nousiainen, CLIC workshop ” Technical Issues, Integration & Cost ” working group Progress on Study of Module Cooling Risto Nousiainen.
Tolerances coming from RF Alexej Grudiev 24 Nov 2014 X-band accelerating structure review.
1 Design and objectives of test accelerating structures Riccardo Zennaro.
Accelerating structure prototypes for 2011 (proposal) A.Grudiev 6/07/11.
1 Error study of non-scaling FFAG 10 to 20 GeV muon ring Shinji Machida CCLRC/RAL/ASTeC 26 July, ffag/machida_ ppt.
Beam dynamics in crab collision K. Ohmi (KEK) IR2005, 3-4, Oct FNAL Thanks to K. Akai, K. Hosoyama, K. Oide, T. Sen, F. Zimmermann.
X-band Based FEL proposal
STATUS OF THE NC BUNCHING RFQ (Sub-task: SC-RFQ) Antonio Palmieri INFN-LNL.
Aaron Farricker 107/07/2014Aaron Farricker Beam Dynamics in the ESS Linac Under the Influence of Monopole and Dipole HOMs.
1 & 2 JUNE 2015 – LLRF – BEAM DYNAMICS WORKSHOP URIOT Didier What is taken into account in simulations LLRF – Beam dynamics Workshop.
Progress in CLIC DFS studies Juergen Pfingstner University of Oslo CLIC Workshop January.
Yingshun Zhu Design of Small Aperture Quadrupole Magnet for HEPS-TF
Review of Alignment Tolerances for LCLS-II SC Linac Arun Saini, N. Solyak Fermilab 27 th April 2016, LCLS-II Accelerator Physics Meeting.
Structure Wakefields and Tolerances R. Zennaro. Parameters of the CLIC structure “CLIC G” (from A. Grudiev) StructureCLIC_G Frequency: f [GHz]12 Average.
A. Aksoy Beam Dynamics Studies for the CLIC Drive Beam Accelerator A. AKSOY CONTENS ● Basic Lattice Sketches ● Accelerating structure ● Short and long.
First evaluation of Dynamic Aperture at injection for FCC-hh
Test Accelerating Structures Designs, Objectives and Critical Issues
RF-kick in the CLIC accelerating structures
Correlated Misalignments Studies for LCLS-II SC Linac
For Discussion Possible Beam Dynamics Issues in ILC downstream of Damping Ring LCWS2015 K. Kubo.
Physics design on the main linac
Wake field limitations in a low gradient main linac of CLIC
Optimisation of single bunch linac for FERMI upgrade
X-band FEL beam dynamics issues
Physics design on Injector-1 RFQ
IHEP-CLIC Collaboration (Beam Dynamics)
Emittance growth AT PS injection
Summary of the test structure design
Update of CLIC accelerating structure design
Progress in the design of a damped an
5th X-Band Structure Collaboration Meeting
Studies on orbit corrections
Beam dynamics requirements on MQT
Yuri Nosochkov Yunhai Cai, Fanglei Lin, Vasiliy Morozov
Bunch Compressor Beam Line Optics
Presentation transcript:

Tolerances: Origins, Requirements, Status and Feasibility R. Zennaro R. Zennaro CLIC meeting 27/04/07

Tolerances of the structures 4 kinds of tolerances: Machining (Δx, Δy, Δz) Assembly (Δx, Δy, Δz) Alignment (Δx, Δy, Δz) Operation [Cooling] (ΔT (t) water in, ΔT (z)) 4 kinds of problems: Beam induced transverse kick (wakefield) RF induced transverse kick RF matching (reflected power) Phase error 2 kinds of technologies: Structures in quadrants Structures in disks Predictable: operational temperature, longitudinal elongation, transverse elongation Unpredictable: water temperature instability, RF power variation

Schematic view of possible errors 9 10 Schematic view of possible errors

10

CLIC_G Courtesy of A. Grudiev Structure Shape Dephasing: Mismatching: Beam dynamics: An error in the cell shape determines a wrong phase advance Reflected power: in a structure a geometrical error introduces a reflection i.e. lower efficiency. Considering the last cell (narrowband; vg=0.83%) , the pass band at -30 dB is ~5 MHz and the computed tolerance (DB) to get S11< -30 dB is ~1.5 micron, if any tuning is applied. B D A P The sensitivity of the phase advance to the main geometrical parameters has been computed for the different cells of the CLIC_G structure. Strong dependence on the group velocity: vg/c(%): 1.66 (first cell) 0.83 (last cell) CLIC_G Courtesy of A. Grudiev

Example of a systematic error: metrology of a structure in quadrant (NDS4_vg2.5_thick) Error (microns) Average cell radius error: +0.0055 Aperture error: negligible

Structure Shape (systematic error) 1 micron error, if systematic, gives a very large error on the average phase advance per cell (~11 deg). Acceptable average phase error (Daniel): ~ 1 deg dφ/dB= (dω/dB)/vg Tuning is required The phase error implies a variation on the effective accelerating field Loaded Unloaded

Example of random (?) errors: CLIC_VG1: RF measurements in KEK B Average phase advance per cell -119.943 degrees / cell Average phase advance per cell -120.424 degrees / cell Single cell phase advance error up to 10 deg, sigma A~ 4.5 deg, sigma B~ 5.6 deg, average phase offset is less then 1 deg, D gradient A~0.3%, D gradient B~0.3% (calculated for syn. phase= 8deg) Courtesy of T. Higo

Structure Shape (random error) Gradient error generated by a Gaussian distribution of the phase; NO average phase error. Acceptable average gradient error: sigma=2% (D. Schulte) DB <17 microns (first cell); 9 microns (last cell)

Structure Shape: Tuning by deformation (push-pull) The tuning is provided by deformation with the push/pull technique. Very conservative approach (all the cells are tuned in one goal): Assuming for the tuning screw a step of 0.5mm and a precision of 15o – 20o, the correction can compensate an error equivalent to DB~1 micron Less conservative approach (cells tuned individually): Tuning range determined by the tuning correction range (0.5 mm ?)

Negligible systematic error+ random errors < 1 Negligible systematic error+ random errors < 1.5 micron (for the matching) No tuning required Systematic error < 1 micron + random errors<1.5 micron All the cells are tuned in one goal Else Individual tuning of each cell

Bookshelf or longitudinal misalignment of half-structure Structure in quadrants problem mainly for the machining and assembly Dz Δz1 ≈ D/a* Δz Δz1 Structure in disks problem mainly for the brazing (assembly); probably easier to achieve

Bookshelf or longitudinal misalignment of half-structure Direct kick calculation Panofsky Wenzel (cross-check) DVx/DVz~0.087*Dz computed DVx/DVz=Dz/(4*a)=0.09*Dz Prediction (Daniel) Equivalent bookshelf angle: α=dz/2a Middle cell of CLIC_G (a=2.75mm) Tolerances: 1micron or 18 μrad

Thermal isotropic expansion Assumption: isotropic dilatation for small variation of the temperature of the cooling water Very conservative approach: same T variation for the full linac (?) Dilatation has two effects on phase: Elongation of the structure; 1D problem, negligible effect Detuning and consequent phase error of each cell; 3D problem, dominant effect requirement The average gradient variation is “equivalent” to 0.2 deg phase jitter(*) (drive beam-main beam phase) (*) In the case of synchronous phase = 8 deg

Conclusions Thanks to: R. Nousiainen, D. Schulte RF mismatching, phasing errors and bookshelf are critical for structure tolerances Tuning of the cells seems to be needed Longitudinal precision in the alignment of the quadrant should be ~ 1 micron Bookshelf for structures in disks requires equivalent tolerances (~ 180 μrad) Variation of the cooling water temperature could generate beam energy variations; this should not be a problem (feedback system) Thanks to: R. Nousiainen, D. Schulte