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Evaluation of the radiation field in the future circular collider detector

The radiation load on a detector at a 100 TeV proton-proton collider, that is being investigated within the Future Circular Collider (FCC) study, is presented. A peak luminosity of 30 1034 cm−2s−1 and a total integrated luminosity of 30 ab−1 are assumed for these radiation studies. A first concept o...

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Detalles Bibliográficos
Autores principales: Besana, Maria Ilaria, Cerutti, Francesco, Ferrari, Alfredo, Riegler, Werner, Vlachoudis, Vasilis
Lenguaje:eng
Publicado: 2016
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevAccelBeams.19.111004
http://cds.cern.ch/record/2198578
Descripción
Sumario:The radiation load on a detector at a 100 TeV proton-proton collider, that is being investigated within the Future Circular Collider (FCC) study, is presented. A peak luminosity of 30 1034 cm−2s−1 and a total integrated luminosity of 30 ab−1 are assumed for these radiation studies. A first concept of the detector foresees the presence of central and forward sub-detectors that provide acceptance up to |η|=6 inside a magnetic field generated by the combination of a central solenoid and two forward dipoles. This layout has been modelled and relevant fluence and dose distributions have been calculated using the FLUKA Monte Carlo code. Distributions of fluence rates are discussed separately for charged particles, neutrons and pho- tons. Dose and 1 MeV neutron equivalent fluence, for the accumulated integrated luminosity, are presented. The peak values of these quantities in the different sub-detectors are highlighted, in order to define the radiation tolerance requirements for the choice of possible technologies. The effect of the magnetic field is also discussed. Two shielding solutions have been conceived to minimise the backscattering from the forward calorimeters to the muon chambers and the forward tracking stations. The two tentative designs are presented and their effectiveness is discussed in terms of 1 MeV neutron equivalent fluence and particle fluence rate reduction.