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Электронный каталог: Atanov, N. - The Mu2e Digitizer ReAdout Controller (DiRAC): Characterization and Radiation Hardness
Atanov, N. - The Mu2e Digitizer ReAdout Controller (DiRAC): Characterization and Radiation Hardness
Статья
Автор: Atanov, N.
Nuclear Instruments & Methods in Physics Research A [Electronic resource]: The Mu2e Digitizer ReAdout Controller (DiRAC): Characterization and Radiation Hardness
б.г.
ISBN отсутствует
Автор: Atanov, N.
Nuclear Instruments & Methods in Physics Research A [Electronic resource]: The Mu2e Digitizer ReAdout Controller (DiRAC): Characterization and Radiation Hardness
б.г.
ISBN отсутствует
Статья
Atanov, N.
The Mu2e Digitizer ReAdout Controller (DiRAC): Characterization and Radiation Hardness / N.Atanov, V.Baranov, Yu.I.Davydov, V.Glagolev, [et al.] // Nuclear Instruments & Methods in Physics Research A [Electronic resource]. – 2024. – Vol. 1068. – P. 169688. – URL: https://doi.org/10.1016/j.nima.2024.169688. – Bibliogr.: 4.
The Mu2e experiment at Fermilab will search for the neutrino-less coherent conversion of a muon into an electron in the field of a nucleus. Mu2e detectors comprise a straw tracker, an electromagnetic calorimeter and a veto for cosmic rays. The calorimeter employs 1348 Cesium Iodide crystals readout by silicon photo-multipliers and fast front-end, and digitization electronics. The digitization board is named DiRAC (Digitizer ReAdout Controller) and 140 cards are needed for the readout of the full calorimeter. The DiRACs are hosted in crates located on the external surface of calorimeter disks, inside the detector solenoid cryostat and must sustain very high radiation and magnetic field so it was necessary to fully qualify it. Several version of prototypes were validated for operation in a high-vacuum (10&sup(−4) Torr) and under a 1T magnetic field. An extensive radiation hardness qualification campaign, carried out with photons, 14 MeV neutron beams, and 200 MeV protons, certified the DiRAC design to sustain doses up to 12 krad, neutron fluences up to ~ 10*1*11 MeV n&sub(eq)/cm*2, and very low occurrences of single-event effects. The qualification campaigns and quality assurance procedures will be reviewed.
ОИЯИ = ОИЯИ (JINR)2024
Спец.(статьи,препринты) = С 344.1 - Методы и аппаратура для регистрации элементарных частиц и фотонов$
Спец.(статьи,препринты) = С 344.3 - Ядерная электроника$
Atanov, N.
The Mu2e Digitizer ReAdout Controller (DiRAC): Characterization and Radiation Hardness / N.Atanov, V.Baranov, Yu.I.Davydov, V.Glagolev, [et al.] // Nuclear Instruments & Methods in Physics Research A [Electronic resource]. – 2024. – Vol. 1068. – P. 169688. – URL: https://doi.org/10.1016/j.nima.2024.169688. – Bibliogr.: 4.
The Mu2e experiment at Fermilab will search for the neutrino-less coherent conversion of a muon into an electron in the field of a nucleus. Mu2e detectors comprise a straw tracker, an electromagnetic calorimeter and a veto for cosmic rays. The calorimeter employs 1348 Cesium Iodide crystals readout by silicon photo-multipliers and fast front-end, and digitization electronics. The digitization board is named DiRAC (Digitizer ReAdout Controller) and 140 cards are needed for the readout of the full calorimeter. The DiRACs are hosted in crates located on the external surface of calorimeter disks, inside the detector solenoid cryostat and must sustain very high radiation and magnetic field so it was necessary to fully qualify it. Several version of prototypes were validated for operation in a high-vacuum (10&sup(−4) Torr) and under a 1T magnetic field. An extensive radiation hardness qualification campaign, carried out with photons, 14 MeV neutron beams, and 200 MeV protons, certified the DiRAC design to sustain doses up to 12 krad, neutron fluences up to ~ 10*1*11 MeV n&sub(eq)/cm*2, and very low occurrences of single-event effects. The qualification campaigns and quality assurance procedures will be reviewed.
ОИЯИ = ОИЯИ (JINR)2024
Спец.(статьи,препринты) = С 344.1 - Методы и аппаратура для регистрации элементарных частиц и фотонов$
Спец.(статьи,препринты) = С 344.3 - Ядерная электроника$