13 research outputs found
Beam-induced Background Simulations for the CMS Experiment at the LHC
Beam-induced background comes from interactions of the beam and beam halo particles with either the residual gas in the vacuum chamber of accelerator or the collimators that define the beam aperture. Beam-induced processes can potentially be a significant source of background for physics analyses at the LHC. This contribution describes the simulation software environment used for this part of the CMS experiment activity and recent beam-induced background simulation results for the Phase-2 CMS operation design
The Pixel Luminosity Telescope: a detector for luminosity measurement at CMS using silicon pixel sensors
The Pixel Luminosity Telescope is a silicon pixel detector dedicated to luminosity measurement at the CMS experiment at the LHC. It is located approximately 1.75 m from the interaction point and arranged into 16 “telescopes”, with eight telescopes installed around the beam pipe at either end of the detector and each telescope composed of three individual silicon sensor planes. The per-bunch instantaneous luminosity is measured by counting events where all three planes in the telescope register a hit, using a special readout at the full LHC bunch-crossing rate of 40 MHz. The full pixel information is read out at a lower rate and can be used to determine calibrations, corrections, and systematic uncertainties for the online and offline measurements. This paper details the commissioning, operational history, and performance of the detector during Run 2 (2015–18) of the LHC, as well as preparations for Run 3, which will begin in 2022
Benchmarking LHC background particle simulation with the CMS triple-GEM detector
In 2018, a system of large-size triple-GEM demonstrator chambers was installed in the CMS experiment at CERN\u27s Large Hadron Collider (LHC). The demonstrator\u27s design mimicks that of the final detector, installed for Run-3. A successful Monte Carlo (MC) simulation of the collision-induced background hit rate in this system in proton-proton collisions at 13 TeV is presented. The MC predictions are compared to CMS measurements recorded at an instantaneous luminosity of 1.5 ×10 cm s. The simulation framework uses a combination of the FLUKA and GEANT4 packages. FLUKA simulates the radiation environment around the GE1/1 chambers. The particle flux by FLUKA covers energy spectra ranging from 10 to 10 MeV for neutrons, 10 to 10 MeV for γ\u27s, 10 to 10 MeV for e, and 10 to 10 MeV for charged hadrons. GEANT4 provides an estimate of the detector response (sensitivity) based on an accurate description of the detector geometry, the material composition, and the interaction of particles with the detector layers. The detector hit rate, as obtained from the simulation using FLUKA and GEANT4, is estimated as a function of the perpendicular distance from the beam line and agrees with data within the assigned uncertainties in the range 13.7-14.5%. This simulation framework can be used to obtain a reliable estimate of the background rates expected at the High Luminosity LHC
Modeling the triple-GEM detector response to background particles for the CMS Experiment
An estimate of environmental background hit rate on triple-GEM chambers is
performed using Monte Carlo (MC) simulation and compared to data taken by test
chambers installed in the CMS experiment (GE1/1) during Run-2 at the Large
Hadron Collider (LHC). The hit rate is measured using data collected with
proton-proton collisions at 13 TeV and a luminosity of 1.5
cm s. The simulation framework uses a combination of the FLUKA
and Geant4 packages to obtain the hit rate. FLUKA provides the radiation
environment around the GE1/1 chambers, which is comprised of the particle flux
with momentum direction and energy spectra ranging from to
MeV for neutrons, to MeV for 's, to
MeV for , and to MeV for charged hadrons.
Geant4 provides an estimate of detector response (sensitivity) based on an
accurate description of detector geometry, material composition and interaction
of particles with the various detector layers. The MC simulated hit rate is
estimated as a function of the perpendicular distance from the beam line and
agrees with data within the assigned uncertainties of 10-14.5%. This simulation
framework can be used to obtain a reliable estimate of background rates
expected at the High Luminosity LHC.Comment: 16 pages, 9 figures, 6 table
Physical Design of the Radiation Shielding for the CMS Experiment at LHC
The design of the radiation shielding for the CMS experiment at the LHC requires a simulation of the radiation environment using a model of the CMS experimental setup, accelerator components and the experimental hall infrastructure. The radiation simulations are used to optimise the design of the CMS detectors components and also the interface of the CMS detector with LHC accelerator. The Beam Radiation Instrumentation and Luminosity Project of CMS is responsible for giving important input into the optimisation and upgrade of radiation shielding used in CMS and also the radiation environment simulations software infrastructure. This contribution describes the organization of this work, the simulation software environment used for this part of CMS experiment activity and recent radiation simulation results used to optimise the forward shielding for CMS
Benchmarking of the Radiation Environment Simulations for CMS Experiment at LHC
Radiation Simulations group of the Beam Radiation Instrumentation and Luminosity Project of the CMS experiment provide for CMS radiation environment and radiation effects simulation and benchmarking of these calculations with CMS data and other data from LHC measuring devices. We present some results of such benchmarking and the reliability analysis of the simulation procedures for radiation environment calculations at the LHC
The Pixel Luminosity Telescope: a detector for luminosity measurement at CMS using silicon pixel sensors
Abstract The Pixel Luminosity Telescope is a silicon pixel detector dedicated to luminosity measurement at the CMS experiment at the LHC. It is located approximately 1.75 m from the interaction point and arranged into 16 “telescopes”, with eight telescopes installed around the beam pipe at either end of the detector and each telescope composed of three individual silicon sensor planes. The per-bunch instantaneous luminosity is measured by counting events where all three planes in the telescope register a hit, using a special readout at the full LHC bunch-crossing rate of 40 MHz. The full pixel information is read out at a lower rate and can be used to determine calibrations, corrections, and systematic uncertainties for the online and offline measurements. This paper details the commissioning, operational history, and performance of the detector during Run 2 (2015–18) of the LHC, as well as preparations for Run 3, which will begin in 2022