6–10 Nov 2023
RIKEN Wako campus
Asia/Tokyo timezone

Session

Topic7-2

10 Nov 2023, 13:30
Administrative Headquarters 2F conference room (RIKEN Wako campus)

Administrative Headquarters 2F conference room

RIKEN Wako campus

2-1 Hirosawa, Wako, Saitama, Japan

Conveners

Topic7-2

  • Helmut Weick (GSI Helmholtz Center for Heavy Ion Research GmbH)

Presentation materials

There are no materials yet.

  1. dan coates
    10/11/2023, 13:30
    Invited Oral

    ISIS neutron source Target Station one (TS1) has been operating for nearly 40 years. To safeguard future reliable operation, a decision was made to upgrade the Target, reflector and, moderators (TRAM) assembly along with the associated plant equipment and controls systems. One of the aims of this project was to take some of the lessons learnt from the construction of the second target station...

    Go to contribution page
  2. Tsunayuki Matsubara (KEK/J-PARC)
    10/11/2023, 14:00
    Contributed Oral

    High intensity neutrino beams have been generated using a proton beam power of up to 540 kW at the J-PARC neutrino facility for the long-baseline neutrino experiment since 2009. A 30 GeV proton beam of about 10^14 protons per pulse is injected using fast extraction to the graphite target. The pions generated are focused by the electric magnetic horns, and neutrinos decayed from the pions are...

    Go to contribution page
  3. Dr Drew Winder (Oak Ridge National Laboratory)
    10/11/2023, 14:15
    Contributed Oral

    The Spallation Neutron Source (SNS) at the Oak Ridge National Laboratory is currently the world's highest power pulsed neutron spallation source. The SNS first reached its design power of 1.4 MW in 2013 and began operating steadily at 1.4 MW in 2018. Part of the delay in reaching steady, reliable 1.4 MW operation was due to the capabilities of the target systems. We are...

    Go to contribution page
  4. Ryan Schultz (Oak Ridge National Laboratory)
    10/11/2023, 14:30
    Contributed Oral

    The Ring Injection Dump (RID) is a high energy beam transport (HEBT) region in the SNS accelerator where extra beam is aborted into a 150 kW water cooled beam stop. The location of the two beams on the adjacent vacuum window is currently not well understood. A new quadrupole magnet is being added to the RID beamline as part of the Proton Power Upgrade (PPU) project, so an imaging system was...

    Go to contribution page
  5. Dr Yun Liu (Oak Ridge National Laboratory)
    10/11/2023, 14:45
    Contributed Oral

    Measurement of the strain waveforms is critical to improving SNS target performance and reliable lifetime, as well as to evaluating the efficacy of strain mitigation techniques such as the injection of helium gas into the mercury flow. As the measurements must take place in a very limited space and in the presence of intense electro-magnetic interference and ionizing radiation, fiber-optic...

    Go to contribution page
  6. Dr Takashi Naoe (Japan Atomic Energy Agency)
    10/11/2023, 15:00
    Contributed Oral

    A liquid mercury target system for the pulsed spallation neutron source is installed in the J-PARC. High-power proton beams of 3 GeV 25 Hz is injected to the liquid mercury to produce neutrons. A mercury target vessel made of 316L stainless steel is severely damaged by cavitation which is caused by the proton beam-induced pressure waves. The thickness of beam window is designed to 3 mm to...

    Go to contribution page
Building timetable...