Overview Step by step procedure to validate the model (slide 1 and 2) Procedure for the Ql / beam loading study (slide 3 and 4)

Slides:



Advertisements
Similar presentations
Tom Powers Practical Aspects of SRF Cavity Testing and Operations SRF Workshop 2011 Tutorial Session.
Advertisements

of LFD Compensation Study S1 Global Cryomodule
J. Branlard ALCPG11 – March 2011 – Eugene OR, USA Results from 9mA studies on achieving flat gradients with beam loading P K |Q L studies at FLASH.
Lorentz force detuning measurements on the CEA cavity
Stephen Molloy RF Group ESS Accelerator Division
On Cavity Tilt + Gradient Change (Beam Dynamics) K. Kubo K. Kubo.
SLHC-PP – WP7 Critical Components for Injector Upgrade Plasma Generator – CERN, DESY, STFC-RAL Linac4 2MHz RF source Thermal Modeling Gas Measurement and.
1 9 mA study at FLASH on Sep., 2012 Shin MICHIZONO (KEK) LCWS12(Sep.24) Shin MICHIZONO Outline I.Achievement before Sep.2012 II.Study items for ILC III.
SRF Results and Requirements Internal MLC Review Matthias Liepe1.
E. KAKO (KEK) 2010' Sept. 10 KEK Global Design Effort 1 Lorentz Force Detuning Eiji Kako (KEK, Japan)
1 Results from the 'S1-Global' cryomodule tests at KEK (8-cav. and DRFS operation) Shin MICHIZONO (KEK) LOLB-2 (June, 2011) Outline I. 8-cavity installation.
XFEL The European X-Ray Laser Project X-Ray Free-Electron Laser Tomasz Czarski, Maciej Linczuk, Institute of Electronic Systems, WUT, Warsaw LLRF ATCA.
RF Cavity Simulation for SPL Simulink Model for HP-SPL Extension to LINAC4 at CERN from RF Point of View Acknowledgement: CEA team, in particular O. Piquet.
LLRF Cavity Simulation for SPL
Grzegorz Jablonski, Technical University of Lodz, Department of Microelectronics and Computer Science XFEL-LLRF-ATCA Meeting, 3-4 December 2007 XFEL The.
Proposed TDR baseline LLRF design J. Carwardine, 22 May 2012.
LLRF ILC GDE Meeting Feb.6,2007 Shin Michizono LLRF - Stability requirements and proposed llrf system - Typical rf perturbations - Achieved stability at.
Recent LFD Control Results from FNAL Yuriy Pischalnikov Warren Schappert TTF/FLASH 9mA Meeting on Cavity Gradient Flatness June 01, 2010.
1Matthias LiepeAugust 2, 2007 LLRF for the ERL Matthias Liepe.
John Carwardine 5 th June 2012 Developing a program for 9mA studies shifts in Sept 2012.
W. 3rd SPL collaboration Meeting November 12, 20091/23 Wolfgang Hofle SPL LLRF simulations Feasibility and constraints for operation with more.
Marc Ross Nick Walker Akira Yamamoto ‘Overhead and Margin’ – an attempt to set standard terminology 10 Sept 2010 Overhead and Margin 1.
W. 5th SPL collaboration Meeting CERN, November 25, 20101/18 reported by Wolfgang Hofle CERN BE/RF Update on RF Layout and LLRF activities for.
L-band (1.3 GHz) 5-Cell SW Cavity High Power Test Results Faya Wang, Chris Adolphsen SLAC National Accelerator Laboratory
1 Simulation for power overhead and cavity field estimation Shin Michizono (KEK) Performance (rf power and max. cavity MV/m 24 cav. operation.
Preparation for Sept 9mA studies: Follow-up items from February J. Carwardine, 22 May 2012.
Test plan for SPL short cryomodule O. Brunner, W. Weingarten WW 1SPL cryo-module meeting 19 October 2010.
Group 6 / A RF Test and Properties of a Superconducting Cavity Mattia Checchin, Fabien Eozénou, Teresa Martinez de Alvaro, Szabina Mikulás, Jens Steckert.
Cold Tuner test overview S1-Global at KEK 5-9 July 2010.
John Carwardine 21 st October 2010 TTF/FLASH 9mA studies: Main studies objectives for January 2011.
Thomas Jefferson National Accelerator Facility Operated by the Southeastern Universities Research Association for the U.S. Department of Energy Kirk Davis.
1 Data Analysis of LLRF Measurements at FLASH Shilun Pei and Chris Adolphsen Nov. 16 – Nov. 20, 2008.
Preliminary Results from First Blade Tuner Tests in HTS Yuriy Pischalnikov Warren Schappert Serena Barbannoti Matteo Scorrano.
John Carwardine 20 April 09 Preliminary planning for Aug/Sept studies.
John Carwardine (Argonne) First Baseline Allocation Workshop at KEK September 2010 Experience from FLASH ‘9mA’ experiments Gradient and RF Power Overhead.
LLRF at FLASH for 9mA Program, ILC08, Nov. 19, 2008 LLRF for the FLASH 9mA Program S. Simrock DESY, Hamburg, Germany.
SPL waveguide distribution system Components, configurations, potential problems D. Valuch, E. Ciapala, O. Brunner CERN AB/RF SPL collaboration meeting.
John Carwardine January 16, 2009 Some results and data from January studies.
GDE meeting Beijing (Mar.27, 2010) 1 DRFS LLRF system configuration Shin MICHIZONO KEK LLRF lack layout for DRFS DRFS cavity grouping HLRF requirements.
Detail plan of S1-Global H. Hayano (KEK),
1 LLRF requirements/issues for DRFS Shin MICHIZONO (KEK) BAW1 (Sep.8, 2010)
Warren Schappert Yuriy Pischalnikov FNAL SRF2011, Chicago.
Overview of long pulse experiments at NML Nikolay Solyak PXIE Program Review January 16-17, PXIE Review, N.Solyak E.Harms, S. Nagaitsev, B. Chase,
Operated by the Southeastern Universities Research Association for the U. S. Department of Energy Thomas Jefferson National Accelerator Facility 6 March.
1 Tuner performance with LLRF control at KEK Shin MICHIZONO (KEK) Dec.07 TTC Beijing (Michizono) S1G (RDR configuration) - Detuning monitor - Tuner control.
RF control and beam acceleration under XFEL conditions Studies of XFEL-type Beam Acceleration at FLASH Julien Branlard, Valeri Ayvazyan, Wojciech Cichalewski,
John Carwardine TDR Writing: FLASH 9mA Experiment.
Longitudinal dynamic analysis for the 3-8 GeV pulsed LINAC G. Cancelo, B. Chase, Nikolay Solyak, Yury Eidelman, Sergei Nagaitsev, Julien Branlard.
LLRF regulation of CC2 operated at 4˚K Gustavo Cancelo for the AD, TD & CD LLRF team.
Latest Results on Beam Loaded Experiments at FLASH/TTF Shilun Pei October 27,
Cost Optimization Models for SRF Linacs
Test of the dressed spoke cavity
dependence on QL can not longer be seen
SCRF 21-25/Apr/2008 Measurement & Calculation of the Lorentz Detuning for the transient response of the resonant cavity Introduction “Two.
Studies Leader Report: 9mA webex meeting, 15th March 2011
RF operation with fixed Pks
Cavity Theory Feng QIU.
Outlook of future studies to reach maximum gradient and current
Test plan of ESS HB elliptical cavity
High Gradient Cavities: Cost and Operational Considerations
LLRF Functionality Stefan Simrock How to edit the title slide
CW Operation of XFEL Modules
High gradients in TESLA nine-cell cavities
First High Power Test of the ESS Double Spoke Cavity package
Accelerator Physics Particle Acceleration
Strategic Communications at TRIUMF
CEPC SRF Parameters (100 km Main Ring)
Used PEP-II 476 MHz Cavities for MEIC Collider Rings
Summary of the maximum SCRF voltage in XFEL
Facility for Research Instrumentation and Accelerator Development
Presentation transcript:

Overview Step by step procedure to validate the model (slide 1 and 2) Procedure for the Ql / beam loading study (slide 3 and 4)

Simulator validation procedure – STEP 1 LOW GRADIENT, BEAM OFF Initial conditions – proceed at low gradient (~10-15 MV/m) – beam off – FB off, AFF off, standard step FF table – no dynamic piezo compensation Check the power hybrid settings (ACC6/ACC7) – cryomodule forward power read outs (ACC6 and ACC7) ? Check that all cavities are set to Q L =3e6 – read backs from DOOCS – cross check with DAQ data – adjust if necessary Check that all cavities are on resonance – read backs from DOOCS – cross check with DAQ data – adjust if necessary Compare cavity gradients – at end of fill time – “calibrate” P K distribution on the model Compare cavity phases – check phase waveforms – “calibrate” simulator by adjusting phase offsets Compare cavity tilts – if any, understand where they come from (cavity detuning ? LFD ? coupler directivity ?)

Simulator validation procedure – STEP 2 HIGH GRADIENT, BEAM OFF Increase gradient – reach nominal operating gradient – define administrative quench limits – turn FB on – turn AFF on – turn piezo dynamic compensation on (if available) For each cavity, check – Pfwd (DAQ waveforms and simulator) – Pref (DAQ waveforms and simulator) – Vcav (DAQ waveforms and simulator) amplitude and phase – Q L (DAQ waveforms and simulator) – Detuning (DAQ waveforms and simulator) Possible model limitations – klystron non-linearities – uncompensated Lorentz force detuning – adjacent cavities coupling effects – limited directivity at couplers (Pfwd, Pref) – thermal effect at circulators (introduces hysteresis effect, non-linearities) HIGH GRADIENT, BEAM ON Turn beam ON – low beam (1mA ?) – Quantify beam loading FF ratio needs adjustment ? Amplitude of beam loading compensation Beam induced detuning – can we run with beam but without FB and AFF ? – can we run with beam but without piezo compensation ? Compare cavity tilts – logged in the DAQ ? – compare with simulator (beam ON / beam OFF) – can we change the beam length ? (100, 200, 300 usec ?) – can we scan the beam time over the RF flat top ? (over the whole 800 usec ?) – compare with energy profile  vector sum calibration Proceed with Ql studies

Procedure for Q L / beam loading studies Initial conditions – Start beam off – all cavities set to Q L = 3e6, zero detuning, nominal gradient – all cavity gradients flat Turn beam ON – 1 mA, (2mA, 3mA) – 200 usec Check gradient tilts – do they match predicted tilts ? – within administrative quench limits ? Adjust ratio for flat Vsum – ratio adjustments as expected ? Check gradient tilts – do they match predicted tilts ? – within administrative quench limits ? Check if cavities are detuned – DAQ data cross check – record individual detuning Proceed with Q L adjustments – one cavity at a time – best if performed open loop (is it possible, is it safe ?) – for each cavity, record: optimal experimental Q L resulting detuning Q L adjustment time (for DAQ offline analysis) – compare with simulator optimal Q L Check Q L of adjacent cavities – tune cav.1, record Q L 1 – tune cav.2, record Q L 2 – re-check Q L 1 – etc… Retune cavities – static detuning (piezo DC offset if available, slow tuner otherwise) – compensate for LFD with piezo (or operate at lower gradient to avoid them) – log all retuning adjustments – re-check QL’s Verify gradient flatness – after all QL’s have been adjusted, FB, AFF on ? – verify that all cavity gradients are flat – verify that the vector sum is flat – verify that the beam profile is flat Turn beam OFF – no Q L adjustment – record cavity tilts  compare with simulation – do we exceed administrative quench limits This procedure assumes the possibility to run beam open loop, with no AFF, no FB Beam compensation should be included in the model

Procedure for Q L / beam loading studies : adjusting Q L without beam If we can’t run beam without FB and without AFF – Turn beam OFF – No FB, no AFF – Set the machine to predicted optimal Q L follow same steps as described above – Measure tilts compare with simulation within administrative limits? – Measure detuning – Compensate for static detuning – Check Q L after retuning adjust if needed – FB on – Turn beam ON – AFF on, beam compensation on – Measure tilts verify gradient flatness