2022Unpublished venueOpen access

The MTA primary beamline description and performance [Slides]

Alex Leandro Pérez Pérez, USDOE Office of Science (SC), High Energy Physics (HEP)

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Abstract

The Muon Test Area (2003) was initially constructed to develop, test, and verify muon ionization apparatus using the 400-MeV proton beam from the Fermilab Linac. Since muon facilities involve the capture, collection and cooling of ~1013 muons at a repetition conclusive tests require ~1013 protons/pulse (full Linac beam): the original concept/request was for a full Linac capability (~1014 p/sec). The beamline designed for MTA experiments, however, includes specialized insertions for linac beam diagnostics and beam measurements, greatly enhancing the functionality and complexity of the beamline. Installation of the beamline was complete fall, 2008. It represents the only facility in which experiments have direct access to a primary beam.

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The Muon Test Area (2003) was initially constructed to develop, test, and verify muon ionization apparatus using the 400-MeV proton beam from the Fermilab Linac. Since muon facilities involve the capture, collection and cooling of ~1013 muons at a repetition conclusive tests require ~1013 protons/pulse (full Linac beam): the original concept/request was for a full Linac capability (~1014 p/sec). The beamline designed for MTA experiments, however, includes specialized insertions for linac beam diagnostics and beam measurements, greatly enhancing the functionality and complexity of the beamline. Installation of the beamline was complete fall, 2008. It represents the only facility in which experiments have direct access to a primary beam.

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Available abstract

The Muon Test Area (2003) was initially constructed to develop, test, and verify muon ionization apparatus using the 400-MeV proton beam from the Fermilab Linac. Since muon facilities involve the capture, collection and cooling of ~1013 muons at a repetition conclusive tests require ~1013 protons/pulse (full Linac beam): the original concept/request was for a full Linac capability (~1014 p/sec). The beamline designed for MTA experiments, however, includes specialized insertions for linac beam diagnostics and beam measurements, greatly enhancing the functionality and complexity of the beamline. Installation of the beamline was complete fall, 2008. It represents the only facility in which experiments have direct access to a primary beam.

Key concepts: Beamline, Linear particle accelerator, Beam (structure), Optics, Physics, Particle accelerator, Nuclear engineering, Cryogenics

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