ALICE Commissioning Successes

Slides:



Advertisements
Similar presentations
First Results from the ERL Prototype (ALICE) at Daresbury David Holder, on behalf of the ALICE team. LINAC'08 Victoria, BC.
Advertisements

ERLP / ALICE: a bit of history Yuri Saveliev. ... how all this started SRS DIAMOND ERLP 4GLS... to greener pastures.... Oh yes ! We get there Hmmmm.
J. Rudolph, Helmholtz-Zentrum Berlin EuCARD 2nd ANNUAL MEETING Slice emittance measurements at the ELBE superconducting RF photoinjector.
1 Bates XFEL Linac and Bunch Compressor Dynamics 1. Linac Layout and General Beam Parameter 2. Bunch Compressor –System Details (RF, Magnet Chicane) –Linear.
LC-ABD P.J. Phillips, W.A. Gillespie (University of Dundee) S. P. Jamison (ASTeC, Daresbury Laboratory) A.M. Macleod (University of Abertay) Collaborators.
Diagnostics and commissioning on ERLP Yuri Saveliev ASTeC CONFORM Project: EMMA Design Review Workshop February 2007, Daresbury Laboratory.
ERLP Overview Hywel Owen ASTeC Daresbury Laboratory.
Commissioning August & September. 2 Agenda 11:20 Coffee 11:30 Introduction Sue S 11:35 Controls (an overview) Brian M 10:55 Controls & Data Acquisition.
ALICE : Superconductive Energy Recovery Linac (ERL)
ALICE Status and News Susan Smith Director of ASTeC, STFC E lectron M odel for M any A pplications.
R. Corsini, CLIC Project Meeting - 24 th May 2013 CTF3 1 CTF3: Highlights of the 1 st run R. Corsini for the CTF3 Team 1.
Thomas Roser RHIC Open Planning Meeting December 3-4, 2003 RHIC II machine plans Electron cooling at RHIC Luminosity upgrade parameters.
Siegfried Schreiber, DESY The TTF Laser System Laser Material Properties Conclusion? Issues on Longitudinal Photoinjector.
ALICE Commissioning Successes S.L.Smith, and of course the rest of the ALICE team!
New Electron Beam Test Facility EBTF at Daresbury Laboratory B.L. Militsyn on behalf of the ASTeC team Accelerator Science and Technology Centre Science.
Modelling of the ALICE Injector Julian McKenzie ASTeC STFC Daresbury Laboratory IOP Particle Accelerators and Beams Group Status and Challenges of Simulation.
Low Emittance RF Gun Developments for PAL-XFEL
ASTRA Injector Setup 2012 Julian McKenzie 17/02/2012.
Recent Experiments at PITZ ICFA Future Light Sources Sub-Panel Mini Workshop on Start-to-End Simulations of X-RAY FELs August 18-22, 2003 at DESY-Zeuthen,
ERHIC design status V.Ptitsyn for the eRHIC design team.
Accelerator Science and Technology Centre Extended ALICE Injector J.W. McKenzie, B.D. Muratori, Y.M. Saveliev STFC Daresbury Laboratory,
1 ALICE and EMMA Yuri Saveliev … and many others at DL and beyond ASTeC, STFC Daresbury Laboratory IOP Particle Accelerators and Beams Annual Conference.
Electron Sources for ERLs – Requirements and First Ideas Andrew Burrill FLS 2012 “The workshop is intended to discuss technologies appropriate for a next.
Christopher Gerth DL/RAL Joint Workshop 28-29/4/04 Modelling of the ERLP injector system Christopher Gerth ASTeC, Daresbury Laboratory.
Commissioning and Utilisation of ERLP David Holder ASTeC, Daresbury Laboratory.
The Next Generation Light Source Test Facility at Daresbury Jim Clarke ASTeC, STFC Daresbury Laboratory Ultra Bright Electron Sources Workshop, Daresbury,
First Electrons at the Fermilab superconducting test accelerator Elvin Harms Asian Linear Collider Workshop 2015, Tsukuba 24 April 2015.
Development of High Current Bunched Magnetized Electron DC Photogun MEIC Collaboration Meeting Fall 2015 October 5 – 7, 2015 Riad Suleiman and Matt Poelker.
J. Corlett. June 16, 2006 A Future Light Source for LBNL Facility Vision and R&D plan John Corlett ALS Scientific Advisory Committee Meeting June 16, 2006.
Construction, Commissioning, and Operation of Injector Test Facility (ITF) for the PAL-XFEL November 12, 2013 S. J. Park, J. H. Hong, C. K. Min, I. Y.
Experience with Novosibirsk FEL Getmanov Yaroslav Budker INP, Russia Dec. 2012, Berlin, Germany Unwanted Beam Workshop.
What did we learn from TTF1 FEL? P. Castro (DESY).
X-band Based FEL proposal
PAL-XFEL Commissioning Plan ver. 1.1, August 2015 PAL-XFEL Beam Dynamics Group.
Bunch Shaping for Future Dielectric Wakefield Accelerators W. Gai Mini-Workshop on Deflecting/Crabbing RF Cavity Research and application in Accelerators.
Development of High Brightness Electron Photoinjectors at ASTeC B.L. Militsyn Accelerator Science and Technology Centre Science & Technology Facility Council,
Operation Status of the RF Systems and Taiwan Photon Source
Capabilities and Programmes of STFC’s Accelerator Science & Technology Centre (ASTeC)
Seesion1 summary Unwanted Beam Workshop (UBW 2012) Dark Current Issues for Energy Recovery Linacs.
Free Electron Laser Studies
An Electron source for PERLE
Beam Commissioning Adam Bartnik.
Linac beam dynamics Linac dynamics : C. Bruni, S. Chancé, L. Garolfi,
Beam dynamics for an X-band LINAC driving a 1 keV FEL
Status of the MAX IV Short Pulse Facility
Sara Thorin, MAX IV Laboratory
Ultrashort (few cycles) Pulse Generation in (IR-THz) FELs
UK-XFEL WP1 – Electron Injector Development
E-XFEL Status and First Beam Results
An X-band system for phase space linearisation on CLARA
Slice Parameter Measurements at the SwissFEL Injector Test Facility
Status and Interest of the X-ray FEL SINAP
Have a chance to operate your own beam at CERN
SuperB Injection, RF stations, Vibration and Operations
BUNCH LENGTH MEASUREMENT SYSTEM FOR 500 KV PHOTOCATHODE DC GUN AT IHEP
Accelerators in a new light
Timing and synchronization at SPARC
Tunable Electron Bunch Train Generation at Tsinghua University
F. Villa Laboratori Nazionali di Frascati - LNF On behalf of Sparc_lab
SCRF for cw operating XFEL
Diagnostics overview and FB for the XFEL bunch compressors
Injector: What is needed to improve the beam quality?
Advanced Research Electron Accelerator Laboratory
Jim Clarke ASTeC Daresbury Laboratory March 2006
Brief Introduction to (VUV/)Soft X-ray FELs
Linac Diagnostics Patrick Krejcik, SLAC April 24, 2002
CLIC Feasibility Demonstration at CTF3
LCLS Injector/Diagnostics David H. Dowell, SLAC April 24, 2002
Introduction to Free Electron Lasers Zhirong Huang
Enhanced Self-Amplified Spontaneous Emission
Presentation transcript:

ALICE Commissioning Successes S.L.Smith, and of course the rest of the ALICE team! I

Contents ALICE introduction Photoinjector commissioning Superconducting module status Commissioning EO and synchronisation Science beyond energy recovery Programme Summary

Accelerator Layout Nominal Gun Energy 350 keV Injector Energy 8.35 MeV Circulating Beam Energy 35 MeV RF Frequency 1.3 GHz Bunch Repetition Rate 81.25 MHz Nominal Bunch Charge 80 pC Average Current 6.5 mA (Over the 100 ms Bunch Train)

Photoinjector Photoinjector

First electrons August 2006 Photoinjector JLab GA Gun ceramic – major source of delay – at Daresbury (~1 year late) Copper brazed joint First electrons August 2006

PI Results Bunch length at 10% of peak value vs. bunch charge RMS geometric emittance vs. bunch charge Horizontal Vertical 1 2 3 4 5 10 20 30 40 50 60 70 80 Bunch Charge, pC 40 ASTRA Emittance (RMS), pi-mm-mrad 35 125ps 30 ASTRA 25 Bunch length @ 0.1 micro metres 20 15 10 5 28ps 10 20 30 40 50 60 70 80 Bunch Charge, pC

Photoinjector: Leaks, leaks and more leaks and even more leaks! Since February 2007 we have had 6 leaks In 2008 we had 2 more major failures of the ceramic to metal braze joints A contamination of the whole injector assembly through cross contamination of a neg pump component in the vacuum cleaning facility!! 2 leaks on a pirani gauge (1 capped on present assembly) Leak on a bleed valve We have yet to have manufactured a reliable large ceramic but 2 on order Operational October 2008!

Injector upgrade Improved vacuum conditions ALICE photocathode gun equipped with a photocathode preparation & exchange facility Improved vacuum conditions Reduction of contamination from caesium ions Improved gun stability under high voltage Reduced time for photocathode changeover, from weeks to hours Higher quantum efficiency Allows practical experiments with photocathodes activated to different electron affinity levels

Cryogenics and Superconducting RF Superconducting modules

Field Emission Radiation Issue Even at 9 MV/m, which is the saturation point of the radiation monitor, it is predicted that the low-level RF electronics, close to the linac, would have a lifetime of only around 1000 hrs. At the operational gradient the lifetime would be much shorter!

SC Cavity Processing Plan Further aggressive processing is now planned: Over longer conditioning periods; Varying frequency, pulse width and pulse repetition rate; CW conditioning (only possible at lower power levels); Possibly condition the cavity when warm; Introduce helium into the vacuum (risky!) High average current module installation (2010)

Commissioning ALICE

ALICE Accelerates Towards Energy Recovery Injector & Booster Operational Together!!!! 24/10/08 Midnight at start of a 1 month shutdown ALICE commissioning team successfully accelerated an electron beam through the superconducting booster module. The electron beam was accelerated through the module to around 4 MeV.

Acceleration through both booster cavities YAG-02 First Beam YAG-03 cavity 1 at 5.5 MV/m, phase shift position at 2.2, cavity 2 at 4.9 MV/m Sunday 23rd November Shift 3 (#862)

Acceleration Through The LINAC Sunday December 7th Acceleration Through the LINAC

First Circulation Success on 13 December 11 MeV operation

Full Energy Recovery 20.8 MeV operation Full energy recovery demonstrated on ALICE 20 December 2008. The accelerator has been tuned for transport of the 20.8 MeV beam. The green and dark blue traces show the reduction to “zero” in RF demand on both linac cavities when the (pale blue) beam is decelerated through the cavities.

Commissioning to Energy Recovery Injector voltage 235 keV (350 keV) (Smaller Stanford cermaic) Booster energy gain 4.8 MeV (8 MeV) (Matched to conservative LINAC gradient) Total Energy 20.8 MeV (35 MeV) (Limited by FE/Conditioning) Bunch charge 20 pC (80pC) (Qe lifetime)

Commissioning ALICE First energy recovery (Dec 2009) Fine tuning Without FEL, installation planned Summer 2009 Fine tuning injector tuning for minimal emittance optimisation of energy recovery at nominal beam parameters beam diagnostics Short pulse commissioning stage longitudinal dynamics, electro-optical diagnostic studies Energy recovery with FEL (Summer 2009) first light ! recovery of a disrupted beam

ALICE : First Energy Recovery no undulator installed minimal energy spread (acceleration on crest) not concerned with longitudinal phase space, bunching and de-bunching nothing particularly difficult here major ALICE milestone

ALICE : Fine Tuning Achieving “full” energy and beam power (25?MeV, 80pC) Injector tuning minimal emittance (slit & quad scans) optimisation of booster cavities phases settings buncher electric field optimisation etc… Difference orbit measurements Setting the required linac phases and beam transport Optimising beam transport Measurements emittance Twiss parameters bunch length (zero-crossing and E/O methods) energy spectra Matching with the model Transverse emittance as measured during the gun commissioning ( too high due to field emission from the cathode and non-uniform QE map ?)

ALICE : Short Pulse Commissioning Initially, no FEL still not installed yet … Longitudinal dynamics Linac phases tuning R56 tuning in ARC 1 & ARC 2 sextupole tuning longitudinal bunch compression setup min bunch length Phase transfer measurements using either BPMs or E/O THz measurements E/O bunch length measurements

EO beamline section Beam profile monitor Beam position monitor Synchrotron radiation diagnostics EO diagnostics table Laser room

THz In ALICE Thursday 15th January

EO Diagnostics and Synchronisation

Electro-optic sampling of Coulomb field probe laser co-propagates with bunch (with transverse offset) Coulomb field of relativistic bunch probe laser encoding of bunch information into laser decoding of information from laser pulse thanks to S. Jamison

UK has leading position in EO longitudinal diagnostics Electro-optic technique for bunch profile and time-of-arrival measurements UK has leading position in EO longitudinal diagnostics highest time resolution demonstrated by UK/Dutch/German collaboration at FLASH ALICE test-bed For testing of modified concepts for real system integration cost-vs-capability becoming a driver >£200k for our best resolution system! (cost mostly in the laser) investigate migration of techniques to fibre laser systems integration with timing distribution systems -profile info highly desirable for even arrival time diagnostics EU-IRUVX funding for further prototype of EO system on ALICE Tests for external laboratories... thanks to S. Jamison

ALICE: Fibre Lasers Oscillators / Clocks R&D in-house build... commercial system... gain medium (Er: fibre) pump laser diodes fibre stretcher (cavity length feedback) polarising elements plus.. Active length stabilisation of distribution optical fibre.. Compare arrival time of outgoing and round trip pulses - RF phase detection ~20fs sensitivity - optical cross-correlation ~1fs (?) thanks to S. Jamison

ALICE: Longitudinal profile feedback studies concept recently proven at FLASH phase or amplitude Arrival time Arrival of what? charge mean or peak current ? development through EU/Marie Curie (in proposal stage) E0, j E0, j Arrival time & beam profile (partial?) more profile data  more “knobs” available motivation behind IR-UVX EO profile investigations We can do it on ALICE ! thanks to S. Jamison

ALICE - not just an Energy Recovery Linac E-BEAM CBS X-ray CBS Wiggler Phase I EO diagnostic 532 nm IR FEL IR FEL 4-6um 4-6um Phase II THz Photogun laser TW Laser Mobile laser

Motor and In Line Gearbox Tunable IR FEL JLAB IR Demo Wiggler Tunability by varying : electron energy (24-35MeV) undulator gap (12-20mm) Motor and In Line Gearbox l = 4-12 mm Encoders

Future Plans Future Plans

Science Beyond Energy Recovery EMMA – the first NS FFAG Accelerator physics research Photoinjector upgrade, load lock system and diagnostics line High average current accelerator module Photocathode research and testing (using the upgraded gun) Linac Transfer Matrix Investigation Beam Tomography @ High Bunch Charges and Low Energy Laser slicing Micro-bunching? Laser Wakefield Acceleration (LWFA) on ALICE CBS X-ray source IR and THz research programme Tissue Culture Laboratory @ ALICE Exciting pump – probe research programme with all ALICE light sources: TW laser (10TW, 100 / 35 fs, 10Hz) IR FEL (~4mm, ~15MW peak, ~1ps, ~10mJ) fs tunable laser THz radiation (broadband) CBS X-ray source (15-30keV, 107 – 108 photons/pulse, <1ps)

THz Programme & Tissue Culture Facility A world-unique facility allowing the effect of high peak power / high rep rate THz on living cells to be investigated. Weightman et al University of Liverpool University of Nottingham THz has important role in security screening

CBS experiment : Phase I Head on 180o photon-electron collisions (relaxed synchronisation requirements) X-ray source characterisation spectrum X-ray pulse duration brightness (number of photons Np ) Electron bunch / laser pulse time jitter shot-to-shot variations in energy spectra and Np better resolution expected in phase II First pump/probe experiment (but this more likely to be done during phase II) -Laser pulse travels through the length of the electron bunch X-ray pulse length ~ electron bunch length relaxed synchronisation requirements First X-ray pulses April 2009

CBS: Phases I & II PHASE I PHASE II Head on 180o photon-electron collisions Side-on 90o photon-electron collisions e- Phase 1 e- Phase 2

Cathode change (ceramic?) Linac module and Gun upgrade ALICE Programme CBS Installation Cathode change (ceramic?) At Risk Maintenance Linac module and Gun upgrade FEL Installation

Summary Accelerator commissioning has now reached a critical stage ALICE has provided the UK with an opportunity to develop generic technologies and skills important to delivery of advance accelerator driven facilities Photoinjector, SC RF, cryogenics etc. ALICE will provide a unique R&D facility in Europe, dedicated to accelerator science & technology development Offering a unique combination of accelerator, laser and free-electron laser sources Enabling essential studies of beam combination techniques Providing a suite of photon sources for scientific exploitation Many thanks to all contributors to this presentation