Photocathode based Electron Sources for Particle Accelerators – Yesterday, Today and Tomorrow B.L. Militsyn STFC ASTeC, UK European Workshop on Photocathodes.

Slides:



Advertisements
Similar presentations
Injection system of the 4GLS light source B.L. Militsyn on behalf of 4GLS team ASTeC STFC Daresbury Laboratory ERL07 Workshop, Daresbury,
Advertisements

High Brightness Electron Source Lab.
The development of ultra bright electron sources: An overview B.L. Militsyn Accelerator Science and Technology Centre Science & Technology Facility Council,
Radiation Physics | ELBE | SRF Photo Injector for Electron- Laser Interaction LA 3 NET conference: Laser applications at accelerators, Mallorca,
SFB Investigation of pulsed spin polarized electron beams at the S-DALINAC PSTP 2013 PSTP Martin Espig – M. ESPIG, J. ENDERS, Y.
ERLP Overview Hywel Owen ASTeC Daresbury Laboratory.
~1m undulator IP Pol. e + source based on Compton scattering with FEL & 4 mirror cavity Low energy electron beam Gamma-ray FEL photon beam LCWS2014 in.
Before aperture After aperture Faraday Cup Trigger Photodiode Laser Energy Meter Phosphor Screen Solenoids Successful Initial X-Band Photoinjector Electron.
Rong Xiang I I Photocathodes for Rossendorf SRF gun Rong Xiang for HZDR SRF-gun team 1 st Topical Workshop on laser based particle.
Progress of SRF and ERL at Peking University Lu Xiangyang Institute of Heavy Ion Physics Peking University.
D.H. Dowell/MIT Talk, May 31, David H. Dowell Stanford Linear Accelerator Center Photocathode RF Guns and Bunch Compressors for High-Duty Factor.
New Electron Beam Test Facility EBTF at Daresbury Laboratory B.L. Militsyn on behalf of the ASTeC team Accelerator Science and Technology Centre Science.
A Design Study of a 100-MHz Thermionic RF Gun for the ANL XFEL-O Injector A. Nassiri Advanced Photon Source For ANL XFEL-O Injector Study Group M. Borland.
ESources Summary T. Kamps, C. Hernandez-Garcia FLS 2012 Workshop – FLS 2012 | Intro to WG eSources | Thorsten Kamps |
Modelling of the ALICE Injector Julian McKenzie ASTeC STFC Daresbury Laboratory IOP Particle Accelerators and Beams Group Status and Challenges of Simulation.
Photocathode 1.5 (1, 3.5) cell superconducting RF gun with electric and magnetic RF focusing Transversal normalized rms emittance (no thermal emittance)
I.V. Bazarov, Multivariate Optimization of High Brightness DC Gun Photoinjector, UCLA Workshop, 8-10 November CHESS / LEPP ERL DC Gun Injector.
Low Emittance RF Gun Developments for PAL-XFEL
High Current Electron Source for Cooling Jefferson Lab Internal MEIC Accelerator Design Review January 17, 2014 Riad Suleiman.
Development of Dielectric PETS Chunguang Jing and Wei Gai ANL and Euclid CLIC workshop 2013.
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,
1 Working Group 5 Summary: High Brightness Electron Guns High Brightness Electron Guns Fay Hannon, Fernando Sannibale 48th ICFA Advanced Beam Dynamics.
CLARA Gun Cavity Optimisation NVEC 05/06/2014 P. Goudket G. Burt, L. Cowie, J. McKenzie, B. Militsyn.
RF scheme of electron linear accelerator with energy MeV Levichev A.E. Budker Institute of Nuclear Physics SB RAS.
Accelerator Science and Technology Centre Extended ALICE Injector J.W. McKenzie, B.D. Muratori, Y.M. Saveliev STFC Daresbury Laboratory,
LDRD: Magnetized Source JLEIC Meeting November 20, 2015 Riad Suleiman and Matt Poelker.
Electron Sources for ERLs – Requirements and First Ideas Andrew Burrill FLS 2012 “The workshop is intended to discuss technologies appropriate for a next.
Velocity bunching from S-band photoinjectors Julian McKenzie 1 st July 2011 Ultra Bright Electron Sources Workshop Cockcroft Institute STFC 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,
FLS2010 Workshop, Stanford, March 1-5, 2010 Florian Loehl (Cornell University) Commissioning of the High Current ERL Injector at Cornell Florian Loehl.
Future Circular Collider Study Kickoff Meeting CERN ERL TEST FACILITY STAGES AND OPTICS 12–15 February 2014, University of Geneva Alessandra Valloni.
Intro to WG, part II T. Kamps, C. Hernandez-Garcia FLS 2012 Workshop – FLS 2012 | Intro to WG eSources | Thorsten Kamps.
김 귀년 CHEP, KNU Accelerator Activities in Korea for ILC.
Page 1 Polarized Electron Sources for Linear Colliders October, 2010 A. Brachmann, J. C. Sheppard, F. Zhou SLAC SLAC October 18-22, 2010.
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.
Rong Xiang I I Dark current measurements at the ELBE SRF gun Rong Xiang, Jochen Teichert, Pengnan Lu, Andre Arnold, Petr Murcek,
Main Technical Issues of theSuper B Injector Main Technical Issues of the Super B Injector SuperB Meeting, Isola d’Elba, May 31st – June 3rd, 2008 D. Alesini,
, Summary of Working Group 1 Linear Colliders and Light Sources C. Christou, M. Dehler.
X-band Based FEL proposal
1 Roman Barday Plans for field emission studies at HZB for BERLinPro Unwanted Beam Workshop BERLinPro.
Electron Beam Test Facility (EBTF) & Photocathode R&D programme at Daresbury Laboratory Deepa Angal-Kalinin ASTeC, Daresbury Laboratory 27 th January’12,
Development of High Brightness Electron Photoinjectors at ASTeC B.L. Militsyn Accelerator Science and Technology Centre Science & Technology Facility Council,
An Electron source for PERLE
S.M. Polozov & Ko., NRNU MEPhI
Beam dynamics simulation with 3D Field map for FCC RF gun
Superconducting RF Photoelectron Source -
UK-XFEL WP1 – Electron Injector Development
Status of the CLIC main beam injectors
BUNCH LENGTH MEASUREMENT SYSTEM FOR 500 KV PHOTOCATHODE DC GUN AT IHEP
Accelerators in a new light
Joint Accelerator Research JGU & HZB
Erdong Wang Brookhaven National Laboratory
Injection facility for Novosibirsk Super Charm Tau Factory
MIT Compact X-ray Source
ERL Main-Linac Cryomodule
ERL working modes Georg Hoffstaetter, Professor Cornell University / CLASSE / SRF group & ERL effort High Current mode High Coherence mode High Buch charge.
Beam Dynamics in a Spilt SRF-Gun
Pulsed Ion Linac for EIC
Studies of Emittance & Lifetime
Superconducting High Brightness RF Photoinjector Design
LCLS Commissioning Parameters
Advanced Research Electron Accelerator Laboratory
Explanation of the Basic Principles and Goals
MEIC Polarized Electron Source
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
Injector for the Electron Cooler
Update on ERL Cooler Design Studies
Presentation transcript:

Photocathode based Electron Sources for Particle Accelerators – Yesterday, Today and Tomorrow B.L. Militsyn STFC ASTeC, UK European Workshop on Photocathodes for Particle Accelerator Applications, 6-8 June 2016, Daresbury, UK

Outline Days before yesterday – discovery of the photo- effect Yesterday – first photocathode based electron sources –DC photocathode guns –RF photocathode guns Today – evolution of photoelectron sources –DC –RF (SRF) –VHF Tomorrow – what do we expect from the future photocathodes 6 June 2016 B.L. Militsyn, EWPPAA, Daresbury, UK

Days before yesterday. Discovery of the Photoeffect. The Nobel Prize in Physics 1921 was awarded to Albert Einstein "for his services to Theoretical Physics, and especially for his discovery of the law of the photoelectric effect". Philipp Eduard Anton von Lenard ( ) Albert Einstein ( ) Heinrich Rudolf Hertz ( ) 6 June 2016 B.L. Militsyn, EWPPAA, Daresbury, UK

Yesterday. SLAC DC photocathode gun 6 June 2016 B.L. Militsyn, EWPPAA, Daresbury, UK Photocathode used,GaAs Maximum polarization40%

Yesterday. Los Alamos Photocathode RF gun 6 June 2016 B.L. Militsyn, EWPPAA, Daresbury, UK Operation Frequency1.3 GHz Photocathode used Cs 3 Sb Peak surface field60 MV/m Bunch charge 12 nC Peak beam current A Beam emittance32 mm · mrad

Yesterday. BNL RF Gun 6 June 2016 B.L. Militsyn, EWPPAA, Daresbury, UK Photoctahode usedCu Beam emittance3 mm · mrad

Today: Very general classification of the photoelectron sources Out of the gun photocathode preparation and exchange with a Load-Lock system Electron emission –Photocathodes Metal Amorphous semiconductor Crystalline semiconductors Electron acceleration –DC high voltage –Radiofrequency acceleration Normal conductive acceleration Superconductive acceleration –VHF field acceleration Normal conductive acceleration Superconductive acceleration 6 June 2016 B.L. Militsyn, EWPPAA, Daresbury, UK

Today: Modern DC gun designed for ERL Maximum voltage achieved – 500 kV Maximum design current – 10 mA Photocathode – GaAs/Sb Photocathode preparation system (not shown) integrated with the gun For protection of the ceramic insulator from field emission and scattered electrons it is made segmented B.L. Militsyn, EWPPAA, Daresbury, UK 6 June 2016

Today: NC RF CLARA Gun-400 H shape coupler Cathode plug and spring retaining plate. Gun Cavity RF probe* Cooling channels 6 June 2016 B.L. Militsyn, EWPPAA, Daresbury, UK

Today. Design parameters of the Gun-400 UnitsOperating mode Beam Repetition Rate100 Hz400 Hz FrequencyGHz RF peak powerMW<10 RF average powerkW10 Gun electric fieldMV/m120100/80 Bunch chargepC Operating modePulsed/Train pulsed Pulsed RF feedbackRequired 6 June 2016 B.L. Militsyn, EWPPAA, Daresbury, UK

Today: The LBNL VHF photocathode gun 6 June 2016 B.L. Militsyn, EWPPAA, Daresbury, UK Photocathode used Metal/Te/Sb

Today: ELBE SRF Photocathode gun 6 June 2016 B.L. Militsyn, EWPPAA, Daresbury, UK RF frequency1.3 GHz RF scheme3.5 cells Operation modeCW Photocathode usedCs 2 Te/Metal

Today: Photocathode Materials ClassMate rial QEResponse time Intrinsic Energy Wave Length GunApplication Normally conducting metals Cu, Mg ’s fs100’s mV – 1’s VUVNC-RF, VHF Low rep rate FELs Super conducting metals Nb,Pb ’s fs100’s mV – 1’s VUVSC-RFHigh rep rate FELs Positive e - affinity Te- based Cs 2 Te ps’s100’s mVUVNC-RF, SC-RF VHF DC High rep rate FELs Positive e - affinity Sb- based Cs 3 Sb etc ps’s100’s mVVisibleDC VHF, SCRF(?) NCRF(???) ERLs, High rep rate FELs Negative e - affinity semiconductor GaAs, etc ’s ps – 100’s ps10’s mV – 100’s mVIR- VisibleDC (XHV)Polarized sources, ERLs 6 June 2016 B.L. Militsyn, EWPPAA, Daresbury, UK

Tomorrow: general requirements for electron accelerators: Beam energy – 100’s keV – GeV’s Bunch peak current – Amps – kA’s –Bunch charge – fC’s – nC’s –Bunch duration – fs’s – ns’s Beam average current – nA’s –A’s –Bunch charge – fC’s – nC’s –Bunch repetition rate – Hz – 100’s MHz Beam energy spread – 0.1 %’s Beam emittance – sub µm’s Beam synchronisation – less than10’s of fs 6 June 2016 B.L. Militsyn, EWPPAA, Daresbury, UK

Compact Linear Accelerator for Research and Applications CLARA VELA RF Photoinjector Test Facility ELECTRONS GENERATED HERE ELECTRONS ACCELERATED AND MANIPULATED INTERACTIONS WITH LASER BEAMS FEL OUTPUT GENERATED FEL OUTPUT STUDIED Notes: 1. CLARA uses European RF frequencies 2. X-band cavity is used for phase space linearisation

CLARA Phase I Commissioning starts September June 2016 B.L. Militsyn, EWPPAA, Daresbury, UK

Tomorrow: Requirements to the photocathodes for the future accelerator High Quantum efficiency High Robustness Low intrinsic emittance Fast response time We are waiting your new ideas! 6 June 2016 B.L. Militsyn, EWPPAA, Daresbury, UK

Thank you for your attention!