Latest Results on Beam Loaded Experiments at FLASH/TTF Shilun Pei October 27,

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
Breakdown Rate Dependence on Gradient and Pulse Heating in Single Cell Cavities and TD18 Faya Wang, Chris Nantista and Chris Adolphsen May 1, 2010.
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.
Development of new power supplies for J-PARC MR upgrade Yoshi Kurimoto (KEK) for J-PARC accelerator group.
XFEL The European X-Ray Laser Project X-Ray Free-Electron Laser Review of LLRF system based on ATCA standard, Dec 3-4, 2007 Piezodriver and piezo control.
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.
E. KAKO (KEK) 2009' Sept. 30 Albuquerque Global Design Effort 1 Cavity Test Items in S1-G Cryomodule Eiji Kako (KEK, Japan)
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
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.
RF system issues due to pulsed beam in ILC DR October 20, Belomestnykh, RF for pulsed beam ILC DR, IWLC2010 S. Belomestnykh Cornell University.
Marc Ross Nick Walker Akira Yamamoto ‘Overhead and Margin’ – an attempt to set standard terminology 10 Sept 2010 Overhead and Margin 1.
Elias Métral, LHC Beam Commissioning Working Group meeting, 08/06/2010 /191 SINGLE-BUNCH INSTABILITY STUDIES IN THE LHC AT 3.5 TeV/c Elias Métral, N. Mounet.
L-band (1.3 GHz) 5-Cell SW Cavity High Power Test Results Faya Wang, Chris Adolphsen SLAC National Accelerator Laboratory
1Ben Constance7 th January 2010 FONT5 December 2009 feedback results During the final shift we ran K1-to-P2 position feedback 151.2ns bunch spacing, quadrupoles.
XFEL The European X-Ray Laser Project X-Ray Free-Electron Laser Review of LLRF system based on ATCA standard, Dec 3-4, 2007 Piezodriver and Piezo Control.
1 Simulation for power overhead and cavity field estimation Shin Michizono (KEK) Performance (rf power and max. cavity MV/m 24 cav. operation.
XFEL The European X-Ray Laser Project X-Ray Free-Electron Laser Review of LLRF system based on ATCA standard, Dec 3-4, 2007 Piezodriver and Piezo Control.
ILC FAST TUNER R&D PROGRAM at FNAL Status Report CC2 Piezo Test Preliminary Results Ruben Carcagno (on behalf of the FNAL FAST TUNER Working Group) 4/5/06.
Cold Tuner test overview S1-Global at KEK 5-9 July 2010.
Multibunch beam stability in damping ring (Proposal of multibunch operation week in October) K. Kubo.
John Carwardine 21 st October 2010 TTF/FLASH 9mA studies: Main studies objectives for January 2011.
1 Franz-Josef Decker 1 Multi-Bunch Operation for LCLS Franz-Josef Decker March 17, Definitions and goals multi-bunch within.
–10.06 Milan Italy LUCX system and dark current (1) LUCX project (2) Phase Ⅰ and results (3) Phase Ⅱ and dark current Liu shengguang and LUCX.
Beam stability in damping ring - for stable extracted beam for ATF K. Kubo.
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.
John Carwardine 13 th April, 2011 Report on the 9mA program.
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.
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.
RF measurements during floating MD in Week 40 3 rd of October 2012 LIU-SPS BD WG 25/10/2012 Participants: T. Argyropoulos, H. Bartosik, T. Bohl, J. Esteban.
Scan of piezo drive trigger delay For this timing scan, we picked an amplitude of 7.5V (a little more than required to give minimum rms vibration as identified.
XFEL The European X-Ray Laser Project X-Ray Free-Electron Laser Wojciech Jalmuzna, Technical University of Lodz, Department of Microelectronics and Computer.
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,
FLASH RF gun developments. Sven Pfeiffer for the LLRF team FEL Seminar Hamburg,
Matthias Liepe. Matthias Liepe – High loaded Q cavity operation at CU – TTC Topical Meeting on CW-SRF
RF control and beam acceleration under XFEL conditions Studies of XFEL-type Beam Acceleration at FLASH Julien Branlard, Valeri Ayvazyan, Wojciech Cichalewski,
Overview Step by step procedure to validate the model (slide 1 and 2) Procedure for the Ql / beam loading study (slide 3 and 4)
John Carwardine TDR Writing: FLASH 9mA Experiment.
SRF Cavities Resonance Control. CW mode of operation (FNAL’s experience). Yu. Pischalnikov W. Schappert FNAL TTC CW SRF Meeting, Cornell University, 12June,
LLRF regulation of CC2 operated at 4˚K Gustavo Cancelo for the AD, TD & CD LLRF team.
XFEL The European X-Ray Laser Project X-Ray Free-Electron Laser Wojciech Jalmuzna, Technical University of Lodz, Department of Microelectronics and Computer.
Control Schemes - Agenda
Fabio, Francesco, Francesco and Nicola INFN and University Bari
Test of the dressed spoke cavity
dependence on QL can not longer be seen
Failure analysis at BEPCII
SCRF 21-25/Apr/2008 Measurement & Calculation of the Lorentz Detuning for the transient response of the resonant cavity Introduction “Two.
S1-G for TTC meeting Global Design Effort
Studies Leader Report: 9mA webex meeting, 15th March 2011
Longitudinal beam parameters and stability
Saturday 21st April 00:33 Interlock during ramp on BLM HV
Outlook of future studies to reach maximum gradient and current
F.Marcellini, D.Alesini, A.Ghigo
Notkestrasse 85, Hamburg, Germany
CLIC Drive Beam Stabilisation
CW Operation of XFEL Modules
High gradients in TESLA nine-cell cavities
“Workshop on Linac Operation with Long Bunch Trains” Summary
ICFA Mini-Workshop, IHEP, 2017
Beam dynamics requirements after LS2
PSB rf Foreseen limitations with 2 E13 p at 2 GeV
Presentation transcript:

Latest Results on Beam Loaded Experiments at FLASH/TTF Shilun Pei October 27,

Introduction Experiments with heavy beam loading were done in September 17-20, Adaptive feed-forward and orbit feedback were not adopted, only feedback was used. And, all of the experiments were tuned manually with manual beam loading compensation. Beam loaded data with piezo on and off was collected. 3mA (1MHz/3nC) pulse currents for longer bunch trains of 800 bunches (800µs) can be ran successfully. 9mA (3MHz/3nC) pulse currents for shorter bunch trains of bunches ( µs) can be ran stably but with few bunch train cuts. 9mA (3MHz/3nC) pulse currents with bunch-trains of close to 2400 bunches (800µs) can be ran but with too many bunch train cuts.

1 st Forward Flat Top Statistics (Measurement Noise Error Subtracted) Red: 1MHz/3nC beam with piezo off; Blue: 3MHz/3nC beam with piezo off; Green: 3MHz/3nC beam with piezo on. With beam (feedback on)Without beam (open loop) September 2009 Measurement January 2009 Measurement Blue: nominal + 100Hz Initial detuning with piezo off; Red: nominal initial detuning with piezo off; Green: nominal – 100Hz initial detuning with piezo off.

2 nd Forward Flat Top Statistics (1) (Measurement Noise Error Subtracted) With beam (feedback on)Without beam (open loop) September 2009 Measurement January 2009 Measurement Red: 1MHz/3nC beam with piezo off; Blue: 3MHz/3nC beam with piezo off; Green: 3MHz/3nC beam with piezo on. Blue: nominal + 100Hz Initial detuning with piezo off; Red: nominal initial detuning with piezo off; Green: nominal – 100Hz initial detuning with piezo off.

2 nd Forward Flat Top Statistics (2) (Measurement Noise Error Subtracted) With beam (feedback on)Without beam (open loop) September 2009 Measurement January 2009 Measurement Red: 1MHz/3nC beam with piezo off; Blue: 3MHz/3nC beam with piezo off; Green: 3MHz/3nC beam with piezo on. Blue: nominal + 100Hz Initial detuning with piezo off; Red: nominal initial detuning with piezo off; Green: nominal – 100Hz initial detuning with piezo off; Black: nominal initial detuning with piezo on.

Probe Flat Top Statistics (1) (Measurement Noise Error Included) With beam (feedback on)Without beam (open loop) September 2009 Measurement January 2009 Measurement Red: 1MHz/3nC beam with piezo off; Blue: 3MHz/3nC beam with piezo off; Green: 3MHz/3nC beam with piezo on. Blue: nominal + 100Hz Initial detuning with piezo off; Red: nominal initial detuning with piezo off; Green: nominal – 100Hz initial detuning with piezo off.

Probe Flat Top Statistics (2) (Measurement Noise Error Included) Red: nominal initial detuning with piezo off (see slide 8 for the corresponding reflection ratio). Black: nominal initial detuning with piezo on (see slide 8 for the corresponding reflection ratio). With beam (feedback on) Without beam (open loop) September 2009 Measurement January 2009 Measurement Red: 1MHz/3nC beam with piezo off; Blue: 3MHz/3nC beam with piezo off (see slide 7 for the corresponding reflection ratio); Green: 3MHz/3nC beam with piezo on (see slide 7 for the corresponding reflection ratio).

Reflected Signal for Beam on Case September 2009 Measurement Cavities in ACC6 with piezo off 3MHz/3nC beam with 1600 bunches Cavities in ACC6 with Piezo on 3MHz/3nC beam with 1500 bunches

Piezo Off with Nominal Initial Detuning Reflected Ratio for Beam off Case Piezo On with Nominal Initial Detuning Piezo works well to reduce the reflection ratio for open loop beam off case as expected. t A January 2009 Measurement

RF Power Overhead Issue September 2009 Measurement Cavities in ACC6 with piezo off 3MHz/3nC beam with 1600 bunches Cavities in ACC6 with Piezo on 3MHz/3nC beam with 1500 bunches

2nd Forward Flat Top Jitter vs Charge Jitter September 2009 Measurement Red: 1MHz/3nC beam with piezo off; Blue: 3MHz/3nC beam with piezo off; Green: 3MHz/3nC beam with piezo on.

Summary With beam on and piezo on/off, the 1st forward flat top jitter stay at the same level as the no beam open loop case, but the 2nd forward flat top jitter will go to much higher value, especially for the piezo on case. Piezo will increase the 2nd forward flat top rf jitter. No matter the beam and the piezo on or off, the probe signal jitter will stay lower than 1%. In addition, with beam on, the jitter for the piezo on case may be lower than that for the piezo off case, which is different from the no beam open loop case and might be caused by the inappropriate initial detuning and the bigger reflection ratio (>30%). For both beam on and off case, the piezo works well to reduce the reflection ratio. Particularly for the beam on case, the piezo reduces the RF power overhead clearly. For the same beam current, the forward flat top jitter is roughly proportional to the bunch charge jitter.