2013
DOI: 10.48550/arxiv.1306.6329
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The International Linear Collider Technical Design Report - Volume 4: Detectors

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Cited by 168 publications
(297 citation statements)
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“…The CEPC will hosts two interaction points (IP) on the main ring, where the detector at each IP records collision data under different center of mass energies varying from √ s = 91.2 GeV as a Z factory to √ s = 240 GeV as a Higgs factory. To fulfill the physics goals, a baseline concept of the detector is developed based on the International Large Detector (ILD) concept [8] with further optimizations for the CEPC environment. From the most inner sub-detector component, the detector concept is composed of a silicon vertex detector, a silicon inner tracker consisting of micro strip detectors, a Time Projection Chamber (TPC), a silicon external tracker, ultra-fine segmented calorimeters, an Electromagnetic CALorimeter (ECAL) and an Hadronic CALorimeter (HCAL), a 3T superconducting solenoid, and a muon detector [4].…”
Section: Detector Design and Simulation Samplesmentioning
confidence: 99%
“…The CEPC will hosts two interaction points (IP) on the main ring, where the detector at each IP records collision data under different center of mass energies varying from √ s = 91.2 GeV as a Z factory to √ s = 240 GeV as a Higgs factory. To fulfill the physics goals, a baseline concept of the detector is developed based on the International Large Detector (ILD) concept [8] with further optimizations for the CEPC environment. From the most inner sub-detector component, the detector concept is composed of a silicon vertex detector, a silicon inner tracker consisting of micro strip detectors, a Time Projection Chamber (TPC), a silicon external tracker, ultra-fine segmented calorimeters, an Electromagnetic CALorimeter (ECAL) and an Hadronic CALorimeter (HCAL), a 3T superconducting solenoid, and a muon detector [4].…”
Section: Detector Design and Simulation Samplesmentioning
confidence: 99%
“…The event samples of e + e − → b b was generated in center of mass energy of 250 GeV by WHIZARD 1.95 [4]. The full Monte Carlo simulation (MC) was done with Mokka based on Geant4 framework with the reference geometry of the International Large Detector (ILD) concept used in the studies of Detailed Baseline Design report [5], ILD v1 o5 model. The model includes silicon pixel and strip detectors, a time projection chamber, precisely segmented electromagnetic and hadron calorimeters (ECAL and HCAL) and a 3.5 Tesla solenoid magnet.…”
Section: Simulation Conditionmentioning
confidence: 99%
“…More recently it has been realised that the particle identification (PID) ability to distinguish different kinds of charged hadrons provides important additional information [1,2,3]. Some proposed detector concepts like ILD [4,5] at the ILC [6] or the CEPC [7] detector offer PID via the specific energy loss (dE/dx) in their gaseous main tracking devices, which could be complemented by time-of-flight (TOF) measurements. For the other detector concepts which rely on silicon tracking only, TOF would be the only possibility for charged hadron PID.…”
Section: Introductionmentioning
confidence: 99%