LLRF Stability Improvements for the Operation of SACLA T. Ohshima*, H. Maesaka, S. Matsubara, Y. Otake RIKEN, SPring-8 center LLRF workshop 2015, Shanghai,

Slides:



Advertisements
Similar presentations
Present status of the laser system for KAGRA Univ. of Tokyo Mio Lab. Photon Science Center SUZUKI, Ken-ichiro.
Advertisements

Tessa Charles Australian Synchrotron / Monash University 1 Bunch Compression Schemes for X-band FELs.
Femtosecond Pump / Probe Operation and Plans at the LCLS
1 Bates XFEL Linac and Bunch Compressor Dynamics 1. Linac Layout and General Beam Parameter 2. Bunch Compressor –System Details (RF, Magnet Chicane) –Linear.
Coherent Radiation from High-Current Electron Beams of a Linear Accelerator and Its Applications S. Okuda ISIR, Osaka Univ Research Institute.
Hard X-ray FELs (Overview) Zhirong Huang March 6, 2012 FLS2012 Workshop, Jefferson Lab.
1 Enhancements to the Linac Coherent Light Source.
R. Akre, P. Emma, P. Krejcik LCLS April 29, 2004 LCLS RF Stability Requirements LCLS Requirements The SLAC Linac.
R. Akre XFEL Short Bunch Measurement and July 26, 2004 LCLS Drive Laser Timing Stability Measurements XFEL Short Bunch Measurement.
RF Synchronisation Issues
RF Systems and Stability Linac Coherent Light Source Stanford Synchrotron Radiation Laboratory Stanford Linear Accelerator Center.
SLAC XFEL Short Bunch Measurement and Timing Workshop 1 Current status of the FERMI project (slides provided by Rene Bakker) Photoinjector laser system.
DESY MHF-p 1 Layout of the Synchronisation System for the VUV-FEL Dipl. Ing. Henning Christof Weddig DESY Hamburg.
Stefan Simrock 3 rd LC School, Oak Brook, IL, USA, 2008, Radio Frequency Systems 1 Timing and Synchronization S. Simrock and Axel Winter DESY, Hamburg,
RF Synchronization, control and stability Takuya Natsui.
ANATAC Meeting Line Length Correction Status 2004-Apr-23.
FEL Beam Dynami cs FEL Beam Dynamics T. Limberg FEL driver linac operation with very short electron bunches.
W.S. Graves, ASAC Review, Sept 18-19, 2003 Accelerator Overview Goals for proposal Description of technical components: injector, linac, compressors, etc.
Progress in CW-Timing Distribution for Future Light Sources RUSSELL WILCOX, GANG HUANG, LARRY DOOLITTLE, JOHN BYRD ICFA WORKSHOP ON FUTURE LIGHT SOURCES.
Volker Schlott SV84, LL-RF Workshop, CERN, October 11 th, 2005 Femto-Second Stable Timing and Synchronization Systems Volker Schlott, PSI Motivation –
Holger Schlarb, DESY Normal conducting cavity for arrival time stabilization.
SPIE, PA-IVKrzysztof Czuba1 Improved fiber-optic link for the phase reference distribution system for the TESLA technology based projects Krzysztof.
Low Emittance RF Gun Developments for PAL-XFEL
Lasers and RF-Timing Franz X. Kaertner
SPPS, Beam stability and pulse-to-pulse jitter Patrick Krejcik For the SPPS collaboration Zeuthen Workshop on Start-to-End Simulations of X-ray FEL’s August.
UED at ASTA: LLRF and triggers Need < 100 fs jitter Currently we measure > 500 fs RMS phase noise in 10 Hz to 10 MHz bandwidth at 476 MHz Excessive phase.
Synchronisation Activities for 4GLS Supported by EUROFEL DS3 G J Hirst CCLRC Central Laser Facility.
LLRF-05 Oct.10,20051 Digital LLRF feedback control system for the J-PARC linac Shin MICHIZONO KEK, High Energy Accelerator Research Organization (JAPAN)
LCLS_II High Rep Rate Operation and Femtosecond Timing J. Frisch 7/22/15.
Yb:YAG Regenerative Amplifier for A1 Ground Laser Hut Rui Zhang ACCL Division V, RF-Gun Group Nov 20, 2015 SuperKEKB Injector Laser RF Gun Review.
Laser stability Takuya Natsui. Oscillator phase lock stability.
14th ESLS RF Workshop ELETTRA / Trieste, Italy / 2010 September The Elettra Storage Ring and Top-Up Operation Emanuel Karantzoulis.
BEPC II TIMING SYSTEM EPICS Seminar Presented by Ma zhenhan IHEP 20.August 2002.
Electron Sources for ERLs – Requirements and First Ideas Andrew Burrill FLS 2012 “The workshop is intended to discuss technologies appropriate for a next.
ATF hardware status - Orbit Stabilization T.Naito(KEK) ATF2 Project meeting Laboratoire de l'Accélérateur Linéaire (LAL) 1.Orbit oscillation.
Krzysztof Czuba1 REFERENCE FREQUENCY DISTRIBUTION SYSTEM FOR THE TESLA TECHNOLOGY BASED PROJECTS Krzysztof Czuba Matthias Felber.
Sept 16-17, 2003 Linac Coherent Light Source Stanford Synchrotron Radiation Laboratory Stanford Linear Accelerator Center Controls.
Lessons Learned From the First Operation of the LCLS for Users Presented by Josef Frisch For the LCLS March 14, 2010.
Summary Timing and Diagnostics 1 Franz X. Kärtner and 2 Steve Jamison 1 CFEL - DESY and MIT, 2 Daresbury.
AWAKE synchronization with SPS Andy Butterworth, Thomas Bohl (BE/RF) Thanks to: Urs Wehrle (BE/RF), Ioan Kozsar, Jean-Claude Bau (BE/CO)
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.
Design of New LLRF System for the SPring-8 Storage Ring T. Ohshima on behalf of RF team of SPring-8-II project LLRF Workshop Shanghai.
Performance of the cERL LLRF System Takako Miura (KEK) LLRF'15, Shanghai, Nov 4, 2015 (T. Miura) 1 Compact ERL (Energy Recovery LINAC)
FLASH RF gun developments. Sven Pfeiffer for the LLRF team FEL Seminar Hamburg,
Integrated phase reference distribution LLRF and laser synchronization system Gang Huang 1, Jin Yang 1,2, Qiang Du 1, Wenhui Huang 2, Yilun Xu 1,2, Larry.
What did we learn from TTF1 FEL? P. Castro (DESY).
Possible LLRF Configuration in ILC Sigit Basuki Wibowo LLRF Workshop, Shanghai - Nov 5, 2015.
Temporal overlapping for HHG- seeded EUV-FEL operation by using EOS-based timing-drift controlling system H. Tomizawa 1,4 *, S. Matsubara 1, T. Togashi.
Sub-10 fs RF Regulation at REGAE Matthias Hoffmann for the LLRF team Low Level Radio Frequency Workshop 2015 Shanghai,
Heung-Sik Kang Pohang Accelerator Laboratory
Applications of transverse deflecting cavities in x-ray free-electron lasers Yuantao Ding SLAC National Accelerator Laboratory7/18/2012.
Status of SPARC synchronization system and possible upgrades
Multi-stage pulse compressor
LCLS_II High Rep Rate Operation and Femtosecond Timing
Multi-bunch Operation for LCLS, LCLS_II, LCLS_2025
LLRF Research and Development at STF-KEK
LLRF'15 Workshop, Shanghai, Nov. 4, 2015
An X-band system for phase space linearisation on CLARA
Status and Interest of the X-ray FEL SINAP
ILC Phase Reference Distribution R&D
Timing and synchronization at SPARC
RF Synchronisation Issues
Gu Qiang For the project team
EuCARD2 proposal LLRF Optimization at FLASH
CEPC RF Power Sources System
LCLS Longitudinal Feedback and Stability Requirements
Injector Topics for Discussion
LCLS Drive Laser Timing Stability Measurements
ATF project meeting, Feb KEK, Junji Urakawa Contents :
LCLS RF Stability Requirements
Presentation transcript:

LLRF Stability Improvements for the Operation of SACLA T. Ohshima*, H. Maesaka, S. Matsubara, Y. Otake RIKEN, SPring-8 center LLRF workshop 2015, Shanghai, Nov. 3-7

OUTLINE 1.Introduction to XFEL facility, SACLA 2.Stability requirements 3.Present situation of RF stability 4.Cause of drifts (humidity & temperature) 5.Counter measures a.Upgrade Humidifier of klystron gallery b.Precise air conditioner for master oscillator room c.Optical length control of transmission line for reference signals 6.Results of counter measures 7.Summary

1. Introduction to SACLA XFEL facility in Japan – Provide coherent X-rays to users with ~0.6mJ, ~10fs, 4keV~15keV, 60pps – Characteristics: 8GeV, thermionic electron gun, C- band accelerator, in-vacuum undulator Multi beam line operation (BL3 & BL2) Newly installed dedicated accelerator for BL1 (EUV region): First lasing on 15 37eV

1. Introduction to SACLA Timing & LLRF system H. Maesaka, et.al, ICALEPCS2009,Kobe

2. Stability requirements RF parameters – Compress 1ns beam from gun to ~10fs after BC3 – use 238, 476, 1428, 2856, 5712 MHz Requirements – to keep FEL power fluctuation within 10%rms at pulse width of 10fs for short and long terms (calc. *) phase stability : < 100fs rms amplitude stability : < 1E-4 rms – Phase relations among reference rfs should be kept constant *H. Tanaka, et. al., Proc. of the 4th annual meeting of PASJ, 613 (2007).

3. Parameter drifts Short term stability 23fs rms measured at RF deflector*  enough for user operation Long term stability We experience parameter drifts *Y. Otake,et. al, Phys. Rev. ST Accel. Beams 16, (2013) Sep. 19, 2013 example: 238cavity phase & laser power for 24hr

4.Cause of drifts (humidity & temperature) kly gallery Large fluctuation of FEL intensity in spring and autumn The variation of humidity is large at those seasons Correlation between humidity & cavity phase humidity before improvement (2012)

– Replace Humidifier from ON/OFF control to Linear Control increase humidification capacity 5. Counter measures a) Humidity Klystron Gallery before (2012)  ~5K after (2015)  ~1K

5. Counter measures b) Precise Air Master Oscillator Room – We use Five reference RFs – The phase relations should be stable – Humidity & Temperature Change of the master oscillator room might affect to the relations master oscillator optical transmitter 5712MHz E/O 1/2 E/O 1/2 E/O 1/3 E/O 1/2 E/O 2856MHz 1428MHz 476MHz 238MHz WDMEDFA+Divider to Local Units

Introducing precise air conditioner to master oscillator room temperature variation < 0.1 K humidity variation < 0.2% p-p after before 5. Counter measures b) Precise air master oscillator room

temperature variation – We use optical transmission system for reference RFs. – Phase Stabilized Optical Fiber < 5ps/K/km – Temperature stabilized housing for optical fiber – No counter measure for humidity change 5. Counter measures c)Optical transmission system

Humidity and temperature variation – Introducing optical length feedback control system presented by Y. Otake 2013 LLRF 5. Counter measures c)Optical transmission system frequency stabilized laser EO: GHz master oscillator EO: 5.712GHz x8 Fiber Stretcher control Faraday rotator mirror Fiber Stretcher output phase det 5.712GHz control Fine Coarse TXU EO: trigger, 5712, 238MHz inter- ferometer inter- ferometer Master oscillator room Local control unit optical fiber

Without Optical Length FB With Optical Length FB daily drift of ~ 0.1ps p-p was reduced to < 0.05ps p-p 5. Counter measures c) Optical Length Control Correlation between humidity and SB phase Trend of humidity and SB phase

6. Result of counter measures Trend graph of 238 cavity phase upgrade kly gallery introduce precidion air master start beam commissioning

7. Summary Counter measures to RF parameter drifts – Stabilize the master oscillator room & klystron gallery – Introduce optical length feedback control transmission lines for reference signals Situation was improved. But there are still parameter drifts – condition of cathode of gun, drift of high voltage pulser used at beam chopper,,, We continue making further efforts

spare

SB LBLB CBCB With feedback Without optical length feedback