LEReC Laser Controls & RF Requirements Brian Sheehy 10/31/13 Laser timing Laser design RF and Control Needs.

Slides:



Advertisements
Similar presentations
PPLN Frequency- Doubling Project Diana Parno Hall A Parity Collaboration Meeting May 17, 2007.
Advertisements

CAVITY LOCK ELECTRONICS Dan Sexton, Sirish Nanda, and Abdurahim Rakhman.
Mostly by Gwyn Williams and the JLab Team, Presented by D. Douglas Working Group 4 Diagnostics & Synchronization Requirements Where we are and what needs.
Lock-in amplifiers Signals and noise Frequency dependence of noise Low frequency ~ 1 / f –example: temperature (0.1 Hz), pressure.
Present status of the laser system for KAGRA Univ. of Tokyo Mio Lab. Photon Science Center SUZUKI, Ken-ichiro.
June 28, 2012 Brian Sheehy Laser and Optical Issues in Gatling Gun Development Brian Sheehy June 28, 2012 I. Laser description for Phase I experiments.
SPEAR3 short pulse development J. Safranek for the SSRL accelerator physics group* Outline: Timing mode fill patterns Short bunches –Low alpha Bunch length.
CHRIS HOVDE, STEVE M. MASSICK and DAVID S. BOMSE
Output to accelerator area drive laser: MHz, sync’d to master RF = 1064 nm ~7 ps pulses ~10 watts average (~120 nJ/pulse) chopper wheel: ~100Hz,
RF / Laser Timing for 5/20/14 Frisch. Requirements, Jitter and Drift Looking for 100fs Pk-Pk measurements – 30fs RMS. (state of the art) Jitter:
Laser to RF synchronisation A.Winter, Aachen University and DESY Miniworkshop on XFEL Short Bunch Measurement and Timing.
Bill White Drive Laser April 16, Drive Laser Commissioning Experience Reminder of requirements on Drive Laser.
Yb Fiber Laser System Xiangyu Zhou 19. Feb
RF Synchronisation Issues
SLAC XFEL Short Bunch Measurement and Timing Workshop 1 Current status of the FERMI project (slides provided by Rene Bakker) Photoinjector laser system.
Linac Laser Notcher Status David Johnson Todd Johnson, Vic Scarpine, Andrea Saewert, John Sobolewski PIP Meeting March 6, 2013 Beams Doc 4306.
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,
WP06_AntennaIF. WP06_AntennaIF 3 principal modules switch amplifier (= ATA ‘PAM’) –includes attenuators (0-60 dB), power detector, and bias tee for the.
David Johnson –APC -.  The Proton Improvement Plan is tasked with Booster upgrades which will increase the Booster throughput required for future operation.
Lock-in amplifiers
RF Synchronization, control and stability Takuya Natsui.
Laser Notcher Pulse Energy Requirements & Demonstration Experiment David Johnson, Todd Johnson, Vic Scarpine.
Front-end amplifiers for the beam phase loops in the CERN PS Alessandro Meoli (CERN BE/RF/FB) Supervised by Heiko Damerau 21 April CERN.
Siegfried Schreiber, DESY The TTF Laser System Laser Material Properties Conclusion? Issues on Longitudinal Photoinjector.
Laser Notcher Status Dave Johnson PIP Meeting April 29, 2014.
October 16-18, 2012Working Group on Space-based Lidar Winds 1 AEOLUS STATUS Part 1: Design Overview.
MODULATION AIDA ESMAEILIAN 1. MODULATION  Modulation: the process of converting digital data in electronic form to an optical signal that can be transmitted.
DMP Product Portfolio Femtosecond Lasers Trestles Ti:Sapphire lasers …… fs; nm, mW Mavericks Cr:Forsterite lasers
Summary of issues. RF-Gun cavity – Disk and washer (DAW) : very fast RF ageing, 2 MeV is not enough. – Quasi travelling wave side couple structure : Lower.
Volker Schlott SV84, LL-RF Workshop, CERN, October 11 th, 2005 Femto-Second Stable Timing and Synchronization Systems Volker Schlott, PSI Motivation –
Simple Multiwavelength Time-Division Multiplexed Light Source for Sensing Applications Thilo Kraetschmer and Scott Sanders Engine Research Center Department.
Performance Testing of a Risk Reduction Space Winds Lidar Laser Transmitter Floyd Hovis, Fibertek, Inc. Jinxue Wang, Raytheon Space and Airborne Systems.
LCLS_II High Rep Rate Operation and Femtosecond Timing J. Frisch 7/22/15.
FLASH II. The results from FLASH II tests Sven Ackermann FEL seminar Hamburg, April 23 th, 2013.
PULSE LASER WIRE Laser pulse storage in an optical cavity as a beam monitor & an X-ray source Kaori Takezawa Kyoto Univ. 2nd Mini-Workshop on Nano Project.
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.
Renovation of the 200 MHz RF system LLRF issues. Cavities redistribution 26 October th LIU-SPS Coordination Meeting 2  2011 : 4 cavities 2 x 4.
FFAG Studies at RAL G H Rees. FFAG Designs at RAL Hz, 4 MW, 3-10 GeV, Proton Driver (NFFAGI) Hz,1 MW, GeV, ISIS Upgrade (NFFAG) 3.
July LEReC Review July 2014 Low Energy RHIC electron Cooling Brian Sheehy Laser and Timing.
Oscillator stability & ASE Reduction
Laser stability Takuya Natsui. Oscillator phase lock stability.
Beam stability in damping ring - for stable extracted beam for ATF K. Kubo.
LCLS LLRF System October 10-13, 2005 LLRF05 B. Hong, R. Akre, A. Hill, D. Kotturi, H. Schwarz SLAC, Stanford, Menlo Park, CA 94025, USA Work supported.
M. Hosaka a, M. Katoh b, C. Szwaj c, H. Zen b M. Adachi b, S. Bielawski c, C. Evain c M. Le Parquier c, Y. Takashima a,Y. Tanikawa b Y. Taira b, N. Yamamoto.
BEPC II TIMING SYSTEM EPICS Seminar Presented by Ma zhenhan IHEP 20.August 2002.
Bill White Commissioning October 9, 2006 Drive-Laser Commissioning Status and Plans Requirements Where do we stand today?
704 MHz warm cavity November 4, 2015 A.Zaltsman: SRF & warm RF components for LEReC1  A single cell 704 MHz warm cavity is used to correct the beam energy.
Tze-Wei Liu Y-C Hsu & Wang-Yau Cheng
Bunch Numbering P. Baudrenghien AB/RF for the LHC/RF team.
SPS 200 MHz LLRF upgrade Part 2: Implementation Philippe Baudrenghien, Grégoire Hagmann,
February 17-18, 2010 R&D ERL Brian Sheehy R&D ERL Laser and laser light transport Brian Sheehy February 17-18, 2010 Laser and Laser Light Transport.
Sasha Gilevich, Alan Miahnahri Drive Laser 11/4/2004 Agenda General Information Project Status Transport Tubes Design.
An H- stripping laser using commercial, diode-pumped Nd:YAG amplifiers Russell Wilcox Laser Stripping Workshop, April 11, 2011.
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.
Free Electron Laser Studies
Status of the SPARC laser and “dazzler” experiments
Status of SPARC synchronization system and possible upgrades
LCLS_II High Rep Rate Operation and Femtosecond Timing
Drive-Laser Commissioning Status and Plans
l 66TH MEETING OF THE ESRF l May 2014 l Author
Status of Synchronization System
Lock-in amplifiers
Present status of the laser system for KAGRA
Fill-pattern Control System for KEKB
Device test stations Multi-probe electrical DC injection and optical input/output Near-field measurement Analogue characteristics 1) 50GHz Network analyzer,
Drive Laser Commissioning Status
LCLS Injector Laser System Paul R. Bolton, SLAC April 24, 2002
Injector Drive Laser Technical Status
小型X線源の性能確認実験計画 高輝度・RF電子銃研究会 広島大学 高エネルギー加速器研究機構 浦川順治
Cooling of C6+ ion beam with pulsed electron beam
Presentation transcript:

LEReC Laser Controls & RF Requirements Brian Sheehy 10/31/13 Laser timing Laser design RF and Control Needs

Bunch structure and beam energy Orbital frequency f 0 ~2 kHz range Macrobunch frequency = ion bunch frequency = 120 x orbital freq RF harmonic #, n; RF freq = n x f 0

Timing Structure Average macrobunch frequency is set at the 60 th harmonic of the ring fundamental f 0 one macro gate per ion bunch varies with ϒ : MHz 60-gate pattern phase-locked to f 0 Microbunch frequency is n th harmonic of f 0 and equal to gun RF freq n varies with ϒ : , for f rf = 84 MHz ± 39 kHz this assures turn-by-turn stability microbunch comb located differently in each bunch relative to bunch center, but does not shift turn-by-turn individual pulses are 750 psec FWHM, <150 psec rise and fall times As long as the microbunch frequency is phase-locked with f 0, the pattern is stable with respect to the ion bunches. The pattern can be ‘rastered’ by shifting that phase (along with gate pattern) OLD PLOT

EOM 1 amplifier 1060 nm SHG Narrow bandwidth CW laser 530 nm Optical Pulse Generator Yb-doped Fiber Amplifier Frequency Doubler (PPKTP or sPPLT) Laser Scheme ~84 MHz Pulser & PLL ~9.3 MHz Pulser & PLL EOM 1 EOM = Electro-optic modulator PLL = phase-locked loop milliwatt6-8 W20 W Fiber coupling

Laser Scheme Front end is a narrowband CW laser, with 2-stage electro-optic modulation, at 2 harmonics of the ring frequency f 0, which depends on the beam energy. ~ 9.3 MHz, or 120f 0 ~84 MHz or nf 0, where n varies with beam energy over [1079, 1108] constrained by SRF cavity tunability of ~ 100 kHz 750 psec FWHM pulses <150 psec rise and fall times Multistage fiber amplifier to 20 W average power peak power 1.2 kW Frequency double to 530 nm in PPKTP or MgO:sPPLT Fiber transport ~30 m from laser building to gun in ring enclosure

Transport Laser room Gun Laser must be located outside of ring area -will likely use the same modular building being used for Coherent electron cooling experiments ~ 30 meter path with multiple bends required. Fiber transport is best option

collimator imaging lenses beamsplitter photodetector monument camera fiber Vertical table Laser cross similar setup at ERL shaper losses 25% over 30 m from laser room Transport From Laser room

Basic Scheme is a low power source electro-optically modulated and then amplified All of the phase and timing information is in the signal sent to the EO modulator Optical pulse shape is determined by the pulse shape sent to EO modulator. Optical pulse train should be detected downstream and phase extracted to correct for drifts Control and RF needs/Timing So for phase locking and basic timing, we need: 1. An 84 MHz pulser with 750 psec flat top, 150 psec rise/fall time pulses pulser could be commercial/custom, but input phase-locked trigger source will have to come from LLRF (subnanosecond,TTL) 2.To generate a digital pattern of 120 gates phase-locked with orbital frequency 3. digital phase measurement similar to ERL’s, with feedback to shift the phases of the 9 MHz and 84 MHz pulsers. May want to do that in 2 locations, laser room & gun location Monitor/control thermal drifts similar to ERL

Control and RF needs/non-Timing Laser control Text based commands passed through serial interface On/off, status readbacks, current settings, EOM bias settings Similar to CeCPoP laser software that Peggy Harvey is developing Cameras GiGE, similar to ERL, for alignment and spot quality monitors Laser Power monitors Can probably port ERL software, use Newport heads Steering mirror controls Newport system a bit buggy, would prefer switching to Thorlabs Some issues?