rich detector
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2020 ◽  
Author(s):  
Luka Santelj ◽  
Ichiro Adachi ◽  
Leonid Burmsistrov ◽  
Rok Dolenec ◽  
Koki Hataya ◽  
...  
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Author(s):  
L. Burmistrov ◽  
I. Adachi ◽  
F. Le Diberder ◽  
R. Dolenec ◽  
K. Hataya ◽  
...  
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2020 ◽  
Vol 1526 ◽  
pp. 012033
Author(s):  
F Brizioli ◽  
R Lollini ◽  
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2020 ◽  
Vol 15 (03) ◽  
pp. C03027-C03027
Author(s):  
M. Lenti
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2020 ◽  
Vol 29 (02) ◽  
pp. 2030003
Author(s):  
Anna Senger

The mission of the Compressed Baryonic Matter (CBM) experiment at the future Facility for Antiproton and Ion Research (FAIR) in Darmstadt is to explore the QCD phase diagram at high net baryon densities likely to exist in the core of neutron stars. The CBM detector system is designed to perform multi-differential measurements of hadrons and leptons in central gold-gold collisions at beam energies between 2 and 11 A GeV with unprecedented precision and statistics. In order to reduce the systematic errors of the lepton measurements, which generally suffer from a large combinatorial background, both electrons and muons will be measured with the same acceptance. Up to now, no di-muon measurements have been performed in heavy-ion collisions at beam energies below 158 A GeV. The main device for electron identification, a Ring Imaging Cherenkov (RICH) detector, can be replaced by a setup comprising hadron absorbers and tracking detectors for muon measurements. In order to obtain a complete picture of the reaction, it is important to measure simultaneously leptons and hadrons. This requirement is fulfilled for the RICH, which has a low material budget, and only little affects the trajectories of hadrons on their way to the Time-of-Flight (TOF) detector. In contrast, the simultaneous measurement of muons and hadrons within the same experimental acceptance poses a substantial challenge. This article reviews the simulated performance of the CBM experiment for muon identification, together with the possibility of simultaneous hadron measurements.


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