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Overview of DESY and Accelerator R&D at the Photo Injector Test facility at DESY in Zeuthen (PITZ) Matthias Gross for the PITZ Collaboration, Chiang Mai, Thailand, November 5 th , 2018 Content: DESY: overview PITZ: introduction;


  1. Overview of DESY and Accelerator R&D at the Photo Injector Test facility at DESY in Zeuthen (PITZ) Matthias Gross for the PITZ Collaboration, Chiang Mai, Thailand, November 5 th , 2018 Content: • DESY: overview • PITZ: introduction; projects

  2. DESY – Overview Deutsches Elektronen-Synchrotron • National research centre of Germany • Member of the Helmholtz Association • Two sites: Hamburg and Zeuthen • Hamburg since 1959, Zeuthen since 1992 DESY Together  2300 employees + more than 3000 guest • scientists from over 40 countries each year Research Topics • Accelerators • Photon Science • Particle Physics / Astroparticle Physics | Overview | 2018 Page 2

  3. Research in Zeuthen Astroparticle Physics • Role of high-energy particles in the cosmic evolution • Neutrino astronomy/cosmology, gamma astronomy, theoretical astroparticle physics, multimessenger astronomy Particle Physics • Search for the fundamental building blocks of nature and their interaction • Experimental and theoretical particle physics Accelerators • Development of tomorrow's accelerators • Photoinjector Test Facility in Zeuthen (PITZ) | Overview | 2018 Page 3

  4. DESY in Zeuthen – Overview Modern research centre • More than 280 employees • International participation in science and research • Construction and development • Mechanical and electronic workshops • Computer centre • Detector development • Libraries, administration, communication • School labs | Overview | 2018 Page 4

  5. Latest Science News from DESY in Zeuthen 12 July 2018: Breakthrough in the search for cosmic particle accelerators • Scientists trace a single neutrino back to a galaxy billions of light years away 13 August 2018: World record – Low-draft electron bunches drive high plasma wakes • Scientists achieve highest ratio of acceleration to deceleration in plasma wakes yet 10 October 2018: First CTA telescope inaugurated • LST-1 makes its debut on the northern Cherenkov Telescope Array site | Overview | 2018 Page 5

  6. PITZ Collaboration Partners (formal contract signed) contract on green photocathodes  Founding partners of PITZ: • INFN Milano (C.Pagani): photocathodes • DESY, HH & Z (leading institute) • INR Troitsk (L. Kravchuk): CDS, TDS, Gun5 • HZB (BESSY) (A. Jankowiak): magnets, vacuum • INRNE Sofia (D. Tonev, G. Asova): EMSY + personnel • MBI (S. Eisebitt): cathode laser • LAL Orsay (A. Stocchi): HEDA1 + HEDA2 • TU Darmstadt (TEMF, T. Weiland, H. DeGersem): simulations • STFC Daresbury (D. Angal-Kalinin, B.Militsyn): phase space tomography  Other national partners: • Thailand Center of Excellence in Physics • Hamburg university : (T. Vilaithong, Ch. Thongbai, S. Rimjaem): personnel - most PhD students; • YERPHI (V. Nikoghosyan) + CANDLE (V. Tsakanov, B. - HGF-Vernetzungsfond; Grigoryan), Yerevan : personnel - generation of short pulses - plasma experiments • HZDR : - BMBF-PC-laser-project between MBI, DESY and HZDR, until ~2009; - collaboration between HZB, HZDR, MBI and DESY in SC-gun-cluster  International partners: • IAP Nizhny Novgorod + JINR Dubna : 3D elliptical laser pulses, THz radiation • INFN Frascati + Uni Roma II (L. Palumbo, M. Ferrario): TDS and E-meter pre-studies | Accelerator R&D at PITZ | Matthias Gross for the PITZ Collaboration | Chiang Mai, Thailand, November 5th, 2018 Page 6

  7. Contact to Laser Experts at DESY Now: main E-XFEL photocathode laser Help to set up short pulse laser program at CMU • DESY Group is dedicated for laser developments around accelerators • Group leader: Ingmar Hartl • Small overview of lasers and activities within the FS-LA Laser Science and Technology Group | Applications of Lasers at Accelerators | Matthias Gross for the PITZ team, 01. November 2018 Page 7

  8. Photo Injector Test facility at DESY, Zeuthen site (PITZ) Development, test and optimization of high brightness electron sources for SC linac driven FELs + applications: • test-bed for FEL injectors, e.g. FLASH and European XFEL ( gun cavities and photo injector subsystems  e.g. lasers ) high brightness  small e tr (projected and slice), lots of beam diagnostics • • further studies  e.g. cathodes : dark current, photoemission, QE, thermal emittance , …  applications like plasma acceleration , THz , UED , … <7 MeV <25 MeV booster Pulse Train Time Structure : RF gun PITZ and EXFEL run bunch trains with up to 600 ( 2700 ) laser pulses • L-band (1.3 GHz) 1.6-cell copper cavity flexible shapes 600  s • Ecath >~60MV/m  7MeV/c e-beams t • 650us x 10Hz  up to 45 kW av. RF power • Cs 2 Te PC (QE~5-10%)  up to 5nC/bunch 100 ms • LLRF control for amp & phase stability • Solenoids for emittance compensation t  t = 1  s (222ns) | Accelerator R&D at PITZ | Matthias Gross for the PITZ Collaboration | Chiang Mai, Thailand, November 5th, 2018 Page 8

  9. Towards ultimate low emittance beams  3D ellipsoidal pulses Simulated slice emittance (1nC) 1.2 60 still WR on lowest emittance slice emittance (mm mrad) (Gaussian) measured projected 1 50 emittances 0.8 40 emittance current (A) M. Krasilnikov et al., PRST-AB 15, (flattop) 100701 (2012) 0.6 30 emittance 0.4 20 (3D- ellipsoidal) 0.2 10 current (flattop) 0 0 z-<z> (mm) -5 -4 -3 -2 -1 0 1 2 3 4 5 6 • Laser shaping  key for optimizing photoinjector brightness . • Ellipsoidal laser shaping benefits high bunch charge beams or CW guns (lower gun gradients).  Two methods to generate 3D ellipsoidal photo cathode laser pulses are under study: • Mironov et al., Appl. Opt . 55 , p. 1630 (2016) • Mironov et al., Laser Phys. Lett. 13 , p. 055003 (2016) | Accelerator R&D at PITZ | Matthias Gross for the PITZ Collaboration | Chiang Mai, Thailand, November 5th, 2018 Page 9

  10. Developing 3D ellipsoidal laser pulses First experimental results – collaboration with IAP Nizhny Novgorod IR Spectrogram  Proof of principle demonstrated with IAP system Pharos laser (single SLM  dual path) at PITZ in 2016 Spectrograph Comparison with simulated e - beam shapes (500pC): similarity in shape Inverted MZ Interferometer 20 SLM Gaussian laser Ellipsoidal laser SLM Flattop laser 10 t (ps) 0 -10 @ EMSY1 @PST.Scr1 -20 -10 -5 0 5 10 x (mm) SLM capabilities at First Measurement J. Good et al., Proc. 38 th FEL Conf., WEP006 (2017) proper transport  Redesign to true double SLM setup • Improved stability: commercial Pharos laser oscillator • Improved shaping capabilities: independent masking in x-y, spectrograph feedback • Next: - experiments to quantify shape preserving FHG conversion with angular chirp - true 3D shaping with Volume Bragg Gratings C. Koschitzki et al., Proc. 9 th IPAC, WEPMF059 (2018) | Accelerator R&D at PITZ | Matthias Gross for the PITZ Collaboration | Chiang Mai, Thailand, November 5th, 2018 Page 10

  11. Development of green cathodes on INFN LASA plug design Collaboration with INFN LASA Milano Total Extracted Charge Total Extracted Charge  T est reliable “ green ” cathodes (K -Cs-Sb 2000 2000 1800 1800 compound) in PITZ RF-Gun (high cathode Extracted charge [C] Extracted charge [C] 1600 1600 1400 1400 1200 1200 gradient + fairly high duty cycle) 1000 1000 800 800 600 600 • First sequential deposition on test sample in week 400 400 No light 200 200 47/2017 (“proof of principle”) 0 0 0 0 480 480 960 960 1440 1440 1920 1920 2400 2400 2880 2880 3360 3360 Time [hours] Time [hours] • Long term measurement QE versus time QE versus time (full light spectrum) - Total extracted charge over more than 3 months 1.2 1.2 broad band LED Laser Driven Light Source • >1000C 1 8 𝑛𝑋/𝑑𝑛² ) power density ( power density ( ~21𝑛𝑋/𝑑𝑛² ) LED LED LDLS LDLS 1.0 1.0 - QE versus time: 0.8 0.8 • QE decrease depends on light power density QE [a.u.] QE [a.u.] (fatigue effect?) 0.6 0.6 • Next: Design new source layout in view of co- 0.4 0.4 No light No light evaporation in the near future 0.2 0.2 - Increase QE 0.0 0.0 0 0 480 480 960 960 1440 1440 1920 1920 2400 2400 2880 2880 3360 3360 - Increase life time Time [hours] Time [hours] | Accelerator R&D at PITZ | Matthias Gross for the PITZ Collaboration | Chiang Mai, Thailand, November 5th, 2018 Page 11

  12. Progress in modelling the photoemission process Collaboration with TU Darmstadt and colleagues at DESY in HH  Photoemission beyond linear region is not well simulated.  Short Gaussian laser case is improved using Core + Halo model.  For long laser pulses more relevant to FELs (e.g. Flattop), agreement is worse  work needed . Collaborations with TU Darmstadt o 3D photoemission modeling o Cathode physics model Best beam emittance located in transition region, needs more accurate photoemission modeling.  Ye Chen et al., NIM A 889 (2018) 129-137.  C. Hernandez-Garcia et al., NIM A 871 (2017) 97-104. | Accelerator R&D at PITZ | Matthias Gross for the PITZ Collaboration | Chiang Mai, Thailand, November 5th, 2018 Page 12

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