Oct 3 – 6, 2022
Cornell University
America/New_York timezone

Contribution List

83 out of 83 displayed
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  1. Georg Hoffstaetter (Cornell University (US))
    10/3/22, 9:00 AM
    Welcome and Introduction
    Presentation

    A welcome to the workshop

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  2. Prof. Donald Hartill (Cornell University)
    10/3/22, 9:20 AM
    Welcome and Introduction
    Presentation

    A welcome to Cornell and the ERL 22 workshop by the laboratory director

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  3. Dr Wolfram Fischer (Brookhaven National Lab)
    10/3/22, 9:30 AM
    Welcome and Introduction
    Presentation

    https://cornell.zoom.us/j/93456110989?pwd=WXVwYU1xaW51cHcrWFROSFdOcEpnQT09

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  4. Dr Stuart Henderson (JLab)
    10/3/22, 9:40 AM
    Welcome and Introduction
    Presentation
  5. Andrew Hutton (Jefferson Lab)
    10/3/22, 9:50 AM
    Welcome and Introduction
    Presentation

    Following the European Strategy process in 2019, five Roadmap Panels were set up to prepare the technologies needed for future accelerators and colliders: high-field magnets, SRF, muon colliders, plasma wakefield accelerators and Energy Recovery Linacs (ERLs). The ERL Roadmap Panel, consisting of ERL experts from around the world, first developed a comprehensive overview of current and future...

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  6. Florian Hug (Mainz University)
    10/3/22, 10:50 AM
    Facility Reports
    Presentation
  7. Hiroshi Sakai (KEK)
    10/3/22, 11:10 AM
    Facility Reports
    Presentation

    Compact ERL (cERL) is a test facility, which was constructed on the ERL Test Facility in KEK. Its aim was to demonstrate energy recovery concept with low emittance, high-current CW beams of more than 10 mA for future multi-GeV ERL. In 2016 and 2018, we successfully operate the CW 1 mA beam in the energy recovery condition. Recently, this cERL was operated to promote a variety of the industrial...

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  8. Axel Neumann (Helmholtz Zentrum Berlin)
    10/3/22, 11:30 AM
    Facility Reports
    Presentation

    Since end of the year 2020 the energy recovery linac (ERL) project bERLinPro of Helmholtz-Zentrum Berlin (HZB) has been officially completed. But what is the status of this facility, the next scientific goals in the framework of accelerator physics at HZB, what are the perspectives? To reflect the continuation of this endeavor and the broadening of applications of this machine from high...

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  9. Walid Kaabi (IJCLab)
    10/3/22, 11:50 AM
    Facility Reports
    Presentation
  10. Georg Hoffstaetter (Cornell University (US))
    10/3/22, 1:10 PM
    Facility Reports
    Presentation
  11. Dr Michaela Arnold (TU Darmstadt)
    10/3/22, 1:30 PM
    Facility Reports
    Presentation

    Institut für Kernphysik, Fachbereich Physik, Technische Universität Darmstadt

    The superconducting Darmstadt linear accelerator S-DALINAC [1] is a thrice-recirculating accelerator for electrons at TU Darmstadt. Since its establishment in 1991, the S-DALINAC was mainly developed and operated by students. Besides the conventional acceleration scheme serving various nuclear-physics experiments,...

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  12. Gustavo Pérez Segurana (CERN)
    10/3/22, 1:50 PM
    Facility Reports
    Presentation

    The 5-pass energy recovery project at CEBAF (ER@CEBAF) would become the first facility to have the energy reach to demonstrate ERL performance in the multi-GeV range. This increment in peak energy from the $1\,\textrm{GeV}$ CEBAF-ER demonstration to the target $\sim7\,\textrm{GeV}$ brings incoherent synchrotron radiation-induced energy loss, presents an invaluable opportunity for multi-pass...

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  13. Ms Aveen Mahon (TRIUMF | UVic)
    10/3/22, 2:10 PM
    Facility Reports
    Presentation

    The TRIUMF electron linear accelerator (e-Linac) was conceived to be one of the two main drivers for the upcoming Advanced Rare Isotope Facility (ARIEL). The e-Linac has been commissioned up to 10 kW of average beam power at 30 MeV, for both CW and pulsed beam. It is envisioned for this facility to eventually be upgraded to an Energy Recovery Linac (ERL), with a preliminary design having...

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  14. Dr Dario Giove (INFN Milano - LASA)
    10/3/22, 2:25 PM
    Facility Reports
    Presentation

    We present the detailed design of a compact light source named BriXSinO. BriXsinO is a dual high flux radiation source Inverse Compton Source (ICS) of X-ray and Free-Electron Laser of THz spectral range radiation conceived for medical applications and general applied research. The accelerator is a push-pull CW-SC Energy Recovery Linac (ERL) based on superconducting cavities technology and...

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  15. Gustavo Pérez Segurana (CERN)
    10/4/22, 8:30 AM
    Beam Dynamics and Instrumentation
    Presentation

    Any proposal for an accelerator facility based upon a multipass energy recovery linac (ERL) must possess a self-consistent match in longitudinal phase space, not just transverse phase space. We therefore present a semianalytic method to determine self-consistent longitudinal matches in any multipass ERL. We apply this method in collider scenarios (embodying an energy spread minimizing match)...

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  16. Felix Schließmann (TU Darmstadt)
    10/4/22, 8:50 AM
    Beam Dynamics and Instrumentation
    Presentation

    In a multi-recirculating energy-recovery LINAC (ERL), electrons are accelerated several times in the same LINAC and are decelerated afterwards in the very same LINAC just as often. Even in the case of a twice-recirculating ERL, there are challenges compared to a single-recirculating ERL: When low injector energies are used, phase slippage leads to significantly different energy gains per LINAC...

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  17. Colwyn Gulliford (Xelera Research)
    10/4/22, 9:10 AM
    Uses and Applications
    Presentation

    The baseline scheme for hadron beam cooling in the Electron Ion Collider (EIC) calls for Coherent electron Cooling (CeC) of the hadrons with non-magnetized electrons at high energy (150 MeV electrons), and additional cooling via conventional bunched beam cooling using a precooler system. The electron beam parameters for these concepts are at or beyond the current state of the art, with...

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  18. Andrew Hutton (Jefferson Lab)
    10/4/22, 9:30 AM
    Beam Dynamics and Instrumentation
    Presentation

    In a recent paper, Valery Telnov proposed a linear collider based on twin axis cavities [1]. In a subsequent presentation, Erk Jensen proposed a modification with intra-bucket energy recovery [2], which eliminates higher order mode excitation. Interestingly, this means that there is no need for large aperture SRF cavities and high-power HOM couplers. The Ghost Collider adopts these ideas, and...

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  19. Rob Apsimon (Cockroft Institute), Robert Apsimon (Lancaster University / Cockcroft Institute)
    10/4/22, 9:50 AM
    Beam Dynamics and Instrumentation
    Presentation
  20. Kevin Andre (CERN)
    10/4/22, 10:30 AM
    Beam Dynamics and Instrumentation
    Presentation

    https://cornell.zoom.us/j/93456110989?pwd=WXVwYU1xaW51cHcrWFROSFdOcEpnQT09

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  21. Bettina Kuske (HZB)
    10/4/22, 10:50 AM
    Beam Dynamics and Instrumentation
    Presentation
  22. Robert Michnoff (Brookhaven National LAb)
    10/4/22, 11:10 AM
    Beam Dynamics and Instrumentation
    Presentation
  23. Miho Shimada (KEK)
    10/4/22, 11:30 AM
    Beam Dynamics and Instrumentation
    Presentation
  24. Steven Brooks (BNL)
    10/4/22, 11:50 AM
    Beam Dynamics and Instrumentation
    Presentation
  25. Dr Raffaella Geometrante (KYMA)
    10/4/22, 12:30 PM
    Presentation

    https://cornell.zoom.us/j/93456110989?pwd=WXVwYU1xaW51cHcrWFROSFdOcEpnQT09

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  26. Dr Ilya Ziberter (Tech-X)
    10/4/22, 12:40 PM
    Presentation
  27. Dr Stephen Coleman (RadiaSoft LLC)
    10/4/22, 12:50 PM
    Presentation
  28. Dr Florian Hug (University of Mainz)
    10/4/22, 1:00 PM
    Presentation
  29. Prof. Vaclav Kostroun (Xelera Research LLC)
    10/4/22, 1:10 PM
    Presentation
  30. Hiroshi Sakai (KEK)
    10/4/22, 1:30 PM
    SRF
    Presentation
    SRF

    A superconducting Compact Energy Recovery Linac (cERL) was constructed in 2013 at KEK to demonstrate energy recovery concept with low emittance, high-current CW beams of more than 10 mA for future multi-GeV ERL. cERL consists of 500 kV DC photocathode gun, the injector cavities, the main linac cavity, which made energy recovery, recirculation loop and the beam dump.Under long-term beam...

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  31. Prof. Florian Hug (JGU Mainz, Institut für Kernphysik)
    10/4/22, 1:50 PM
    SRF
    Presentation
    SRF
  32. Axel Neumann (Helmholtz Zentrum Berlin)
    10/4/22, 2:10 PM
    SRF
    Presentation
    SRF

    The energy recovery linac (ERL) at Helmholtz-Zentrum Berlin (HZB) is in the final stage of assembly and follow-up commissioning of the injector beam line. This injector consists of a 1.4\lamba/2 cell SRF photo-injector and a three two cell Booster cryomodule, the latter based on a modified design of the Cornell injector cavity shape. The injector was designed for a final beam current of 100...

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  33. Ramona Leewe (Triumf)
    10/4/22, 2:30 PM
    SRF
    Presentation
    SRF
  34. Taro Konomi (FRIB)
    10/4/22, 2:50 PM
    SRF
    Presentation
    SRF

    KEK has been designing the 10 mA class ERL-EUV light source accelerator. The main linac uses 9-cell superconducting cavities with beamline HOM damper. The target accelerating gradient is 12.5 MV/m. The 9-cell cavity is designed from experience of the KEK compact ERL (cERL) main linac. The cERL main linac was designed to suppress the HOM-BBU with beam current of 100mA by enlarging the iris...

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  35. JOSEPH GRAMES (JEFFERSON LAB)
    10/4/22, 3:40 PM
    Electron Sources
    Presentation

    Extending the charge lifetime of today’s spin polarized GaAs photoelectron guns from hundreds to thousands of Coulombs is a reasonable expectation for long-duration operation at milliampere beam current. In this presentation I will describe some of the topics frequently considered to achieve this goal, and will make quantitative comments about their proven or proposed likelihood for...

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  36. Alice Galdi (Universita degli Studi di Salerno), Alice Galdi
    10/4/22, 4:00 PM
    Electron Sources
    Presentation

    Cs3Sb and related alkali antimonide compounds are high efficiency semiconductor photocathodes that can be operated with visible light and possess quantum efficiency of the order of 1-10% at green light wavelengths. Use of these photocathodes in modern linear accelerators is desirable thanks to their potential to generate high brightness electron beams. However, the ultimate brightness of a...

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  37. Hisato Yamaguchi (LANL)
    10/4/22, 4:20 PM
    Electron Sources
    Presentation
  38. Mengjia Gaowei (BNL)
    10/4/22, 4:40 PM
    Electron Sources
    Presentation

    Attaining high quantum yield, low emittance, and long lifetime from an alkali antimonide photocathode has remained a sustained focus in recent years, due especially to the need for electron beams of high average current for ERL-based electron cooling systems, synchrontron radiation sources, electron ion colliders and other applications. The ongoing development of photocathodes is motivated by...

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  39. Zhentang Zhao
    10/5/22, 8:30 AM
    Uses and Applications
    Presentation

    https://cornell.zoom.us/j/93456110989?pwd=WXVwYU1xaW51cHcrWFROSFdOcEpnQT09

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  40. Tobias Beck (FRIB, MSU)
    10/5/22, 8:50 AM
    Uses and Applications
    Presentation

    The electromagnetic interaction of atomic nuclei with photons is a well-understood process that provides model-independent access to their properties. Consequently, photonuclear-reaction studies below and above the particle separation threshold have been a driving force in the study of the nuclear force for decades. Around the turn of the century, the field experienced a renaissance with the...

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  41. Erdong Wang
    10/5/22, 9:10 AM
    Uses and Applications
    Presentation

    IntraBeam Scattering (IBS) and other diffusion mechanisms in the EIC Hadron Storage Ring (HSR) degrade the beam emittances during a store, with growth times of about 2 hours at the two nominal proton energies of 275 GeV and 100 GeV. Strong Hadron Cooling (SHC) maintains good beam quality and high luminosity during long collision stores. A novel cooling method – Coherent electron Cooling...

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  42. Prof. Florian Hug (JGU Mainz, Institut für Kernphysik), Florian Hug (Mainz University), Kurt Aulenbacker (Mainz University)
    10/5/22, 9:30 AM
    Uses and Applications
    Presentation
  43. Norio Nakamura (High Energy Accelerator Organization (KEK))
    10/5/22, 9:50 AM
    Uses and Applications
    Presentation

    In extreme ultraviolet (EUV) lithography, high volume manufacturing recently started using a laser-produced plasma (LPP) source of 250-W power at 13.5 nm. However, development of a high-power EUV light source is still very important to overcome stochastic effects with a high throughput. The required EUV power to realize the 3-nm node and beyond with a high speed of future scanners is estimated...

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  44. Luca Serafini (INFN)
    10/5/22, 10:30 AM
    Uses and Applications
    Presentation

    https://cornell.zoom.us/j/93456110989?pwd=WXVwYU1xaW51cHcrWFROSFdOcEpnQT09

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  45. Dr I.V. Konoplev (1. JAI, University of Oxford, Oxford, UK. 2.Department of Physics, Sevastopol State University, Russia)
    10/5/22, 10:50 AM
    Uses and Applications
    Presentation

    Energy-frontier particle accelerators are among the most exciting, complex, challenging, and expensive research instruments performing high precision measurements confirming the fundamentals of the physics and broadening new research horizons. Currently the highest energy machines, from multi-GeV to several TeV, (ILC, FCC, CLIC) capable of searching for the most basic building blocks of matter...

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  46. Vladimir Litvinenko (Stony Brook University)
    10/5/22, 11:10 AM
    Uses and Applications
    Presentation
  47. Dr Jan Bernauer (Stony Brook University), Richard Milner (MIT)
    10/5/22, 11:30 AM
    Uses and Applications
    Presentation
  48. Dmitry Kayran (Brookhaven National Laboratory)
    10/5/22, 11:50 AM
    Uses and Applications
    Presentation
  49. Maud Baylac (IJCLab)
    10/5/22, 1:10 PM
    Electron Sources
    Presentation
  50. Omer Rahman (BNL)
    10/5/22, 1:30 PM
    Electron Sources
    Presentation
  51. Xiaofeng Gu (BNL), Xiaofeng Gu
    10/5/22, 1:50 PM
    Electron Sources
    Presentation
  52. Rick van den Berg (Technische Universiteit Eindhoven)
    10/5/22, 2:10 PM
    Electron Sources
    Presentation

    At Eindhoven university a high repetition rate thermionic injector is being built. The injector is capable of supplying electron bunches at a repetition rate of 1.5 GHz, which can be used for x-ray generation.
    The electron source generates a continuous beam with a high current and low emittance through thermionic emission. The continuous electron beam is then chopped into a pulsed beam by a...

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  53. Taro Konomi (FRIB)
    10/5/22, 2:45 PM
    SRF
    Presentation
    SRF

    Superconducting radio-frequency (SRF) electron guns are attractive for delivery of beams at a high bunch repetition rate with a high accelerating field. KEK has been developing the SRF gun to demonstrate basic performance. The SRF gun consists of 1.3 GHz and 1.5 cell SRF gun cavity and K2CsSb photocathode coated on 2K cathode plug. In the vertical test, the surface peak electric field and the...

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  54. Liana Shpani
    10/5/22, 3:05 PM
    SRF
    Presentation
    SRF
  55. Robert Rimmer (JLab)
    10/5/22, 3:25 PM
    SRF
    Presentation
    SRF
  56. Ramona Leewe (Triumf), Ramona Leewe (Triumf)
    10/6/22, 8:30 AM
    SRF
    Presentation
    SRF
  57. Nilanjan Banerjee (The University of Chicago)
    10/6/22, 8:50 AM
    SRF
    Presentation
    SRF

    The Cornell BNL ERL Test Accelerator (CBETA) is the first machine which achieved multi-pass energy recovery employing superconducting cavities. While SRF cavities operated with a narrow bandwidth reduce the overall power consumption of the main linac, maintaining stable field required for energy-recovery in the presence of microphonics detuning becomes a challenging task. We discuss the...

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  58. Mr Carmelo Barbagallo (IJCLab - Université Paris-Saclay)
    10/6/22, 9:10 AM
    SRF
    Presentation
    SRF

    Higher order modes (HOMs) damping is a crucial issue for the next generation of high-current accelerators. Beam-induced HOMs can store sufficient energy in the superconducting RF (SRF) cavities giving rise to beam instabilities and increasing the heat load at cryogenic temperature. To limit these effects, the use of HOM couplers on the cutoff tubes of SRF cavities becomes crucial to absorb...

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  59. Nik Shipman (CERN)
    10/6/22, 9:30 AM
    SRF
    Presentation
    SRF
  60. 10/6/22, 9:50 AM
    Presentation
    SRF
  61. Rong Xiang (Helmholtz-Zentrum Dresden-Rossendorf)
    10/6/22, 10:30 AM
    Electron Sources
    Presentation

    https://cornell.zoom.us/j/93456110989?pwd=WXVwYU1xaW51cHcrWFROSFdOcEpnQT09

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  62. Irina Petrushina (Stony Brook University)
    10/6/22, 10:50 AM
    Electron Sources
    Presentation
  63. Feng Zhou (SLAC)
    10/6/22, 11:10 AM
    Electron Sources
    Presentation
  64. Erdong Wang
    10/6/22, 11:30 AM
    Presentation
  65. Meghan McAteer (Helmholtz-Zentrum Berlin), Dr S.A. Bogaz (JLab, USA)
    10/6/22, 11:45 AM
  66. Daniele Sertore (INFN Milano - LASA)
    Poster Session
    Poster

    We present a proposal related to the development of a High Brightness Beams Test Facility (HB2TF) at the INFN-LASA laboratory close to Milan (Italy).

    The Test Facility will allow to carry out experiments with the high current high brightness CW electron beam in frontier areas of accelerator physics.

    The Test Facility setup will comprise a high-performance laser driven DC Gun (using...

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  67. Yuhong Zhang (Jefferson Lab)
    Poster Session
    Poster

    A γ-γ collider has long been considered an option for a Higgs Factory. Such colliders rely on Compton back-scattering for generating γ photons. The present proposals all choose a thick laser target for scattering. In this paper, we present a new approach for a γ-γ collider utilizing a thin laser target and energy recovery linac for driving the electron beam. This new concept eliminates useless...

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  68. Vasiliy Morozov (Oak Ridge National Lab)
    Poster Session
    Poster

    We present a new concept of a compact high-power linear proton accelerator with an average power of 10 MW at a kinetic beam energy of 1 GeV. Acceleration is accomplished in several stages. In each stage, the beam is recirculated a few times through the same set of SRF cavities. The energy range, cavity type, number of cavities and number of beam recirculations of each stage are optimized to...

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  69. Xiaofeng Gu
    Electron Sources
    Presentation

    Electron cooling of ion beams employing rf-accelerated electron bunches was successfully used for the RHIC physics program in 2020 and 2021. Electron cooler LEReC uses a high-voltage photoemission electron gun with stringent requirements for beam current, beam quality, and stability. The electron gun has a photocathode with a high-power fiber laser, and a novel cathode production, transport,...

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  70. Tobias Beck (FRIB, MSU)
    Uses and Applications
    Presentation

    The electromagnetic interaction of atomic nuclei with photons is a well-understood process that provides model-independent access to their properties. Consequently, photonuclear-reaction studies below and above the particle separation threshold have been a driving force in the study of the nuclear force for decades. Around the turn of the century, the field experienced a renaissance with the...

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  71. Simone Di Mitri (Elettra Sincrotrone Trieste)
    Beam Dynamics and Instrumentation
    Presentation

    So far, IBS has not been observed in single pass electron accelerators because charge density orders of magnitude higher than in storage rings would be needed. We show that such density is now available at high brightness electron linacs for free-electron lasers (FELs).We report measurements of the beam energy spread in the FERMI linac in the presence of the microbunching instability, which...

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  72. Irina Petrushina (Stony Brook University)
    Electron Sources
    Presentation

    High-current low-emittance CW electron beams are of great importance for the existing and future DOE facilities, medical, industrial and security applications. The CW superconducting radiofrequency (SRF) electron photoinjector is one of the most advanced, but also one of the most challenging, technologies promising to deliver such beams. While SRF technology is paving the way for future...

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  73. Sebastian Diego Walter Taubert (JGU Mainz, Institut für Kernphysik)
    Poster Session
    Poster

    The Mainz Energy-recovery Superconducting Accelerator (MESA) at the Institut für Kernphysik der Johannes Gutenberg-Universität Mainz will be commissioned in 2023. Detailed simulations of possible beam optics can be helpful to prepare for this process in order to speed up actual commissioning. The particle tracking code OPAL was chosen as a toolbox to perform these simulations as it handles...

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  74. Heung-Sik Kang (Pohang Accelerator Laboratory), Dr Inhyuk Nam (PAL)
    Poster Session
    Poster

    The PAL-XFEL based on S-band normal conducting linac has demonstrated excellent timing stability and unprecedented peak brightness, outperforming other XFEL facilities since its start of user service operation in June 2017. Based on superconducting RF technology, CW XFEL will be on the horizon, increasing the average brightness by four orders of magnitude from pulsed XFEL; LCLS-II in the USA...

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  75. Oleksiy Fomin (Université Paris-Saclay, CNRS/IN2P3, IJCLab)
    Poster Session
    Poster

    The PERLE collaboration is developing a high power (with a current of up to 20 mA of 500 MeV electrons) ERL machine with three acceleration and three deceleration passes through two cryo-modules. Here we present the design of the first stage of the this machine with one cryo-module that would demonstrate the six-passes operation at a high current with a maximal energy of 250 MeV. All the...

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  76. Mengjia Gaowei (BNL)
    Electron Sources
    Presentation
  77. Quantang Zhao (Institute of modern physics, Chinese academy of sciences)
    Poster Session
    Poster

    A project for a polarized electron-ion collider in China (EicC) is planned based on the high intensity heavy ion accelerator facility (HIAF), which is currently under con-struction. According to the electron beam parameters from the white-paper of EicC, two electron injectors are required, one is polarized electron beam for the collider and another one is for the energy recovery linac (ERL)...

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  78. Joe Grames (JLab)
    Electron Sources
    Presentation
  79. Igor Pinayev (Brookhaven National Laboratory)
    Beam Dynamics and Instrumentation
    Presentation

    The essence of the ERL operation implies that at least two beams (accelerated and decelerated) are co-propagating in the same vacuum vessel and each beam has its own trajectory. The existing beam position monitors measure only “average” trajectory but not that of an individual beam, unless the time separation between bunches is so large that one can resolve individual bunches.
    It was...

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  80. Alice Galdi
    Electron Sources
    Presentation

    https://cornell.zoom.us/j/93456110989?pwd=WXVwYU1xaW51cHcrWFROSFdOcEpnQT09

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  81. Nilanjan Banerjee
    SRF
    Presentation
    SRF
  82. Fanglei Lin (ORNL), Dr Vasiliy Morozov (ORNL)
    Poster Session
    Poster

    We propose to develop an energy-recovery-linac (ERL)-based X-ray free-electron laser (FEL). Taking advantage of the demonstrated high-efficiency energy recovery of the beam power in the ERL, the proposed concept offers the following benefits: i) recirculating the electron beam through high-gradient SRF cavities shortens the linac, ii) energy recovery in the SRF linac saves the klystron power...

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  83. Felix Glöckner (Helmholz Zentrum Berlin)
    Poster Session
    Poster

    The VSR (Variable pulse length Storage Ring) demo module is a prototype for the superconducting upgrade of HZB’s BESSY II. The module houses two 1.5 GHz superconducting cavities operated at 1.8K in continuous wave (CW) mode. Each cavity has five water cooled Waveguide HOM Absorbers with high thermal load (450 W), which requires them to be water cooled. This setup introduces several design...

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