The introduction of picosecond time information in the LHCb ring-imaging Cherenkov (RICH) detectors during LHC Run 4 will allow the primary vertex time (PV t0) to be estimated using only RICH detector information. The presented method can be integrated into the RICH reconstruction algorithm to determine the PV t0. This PV t0 is a necessary input for the application of a time gate around the predicted photon time-of-arrival for each track, which reduces out-of-time photon background from other tracks and improves particle identification (PID) performance. In the RICH reconstruction, each photon object (PO), which is a possible association of a photon detector hit to a particle track, has a PV assigned to it. However, only a fraction of POs is correct and the resolution of the RICH PV t0 strongly depends on the fraction of correct POs for the PV, called the PV purity. To improve the PV purity while maintaining sufficient photon statistics, two PO selection criteria are introduced: the PO signal amplitude and the selection of POs uniquely associated with a pixel hit. The resulting increase in PV purity is 34 % for each selection criteria, while maintaining more than 20 POs for 98 % and 95 % of the PVs in the sample for the first and second selection respectively.
Keizer, F., Malentacca, L. (2025). Primary vertex time reconstruction using the LHCb ring-imaging Cherenkov detectors. Intervento presentato a: 27th International Conference on Computing in High Energy and Nuclear Physics, CHEP 2024 - 19 October 2024 - 25 October 2024, Krakow, Poland [10.1051/epjconf/202533701178].
Primary vertex time reconstruction using the LHCb ring-imaging Cherenkov detectors
Malentacca L.
2025
Abstract
The introduction of picosecond time information in the LHCb ring-imaging Cherenkov (RICH) detectors during LHC Run 4 will allow the primary vertex time (PV t0) to be estimated using only RICH detector information. The presented method can be integrated into the RICH reconstruction algorithm to determine the PV t0. This PV t0 is a necessary input for the application of a time gate around the predicted photon time-of-arrival for each track, which reduces out-of-time photon background from other tracks and improves particle identification (PID) performance. In the RICH reconstruction, each photon object (PO), which is a possible association of a photon detector hit to a particle track, has a PV assigned to it. However, only a fraction of POs is correct and the resolution of the RICH PV t0 strongly depends on the fraction of correct POs for the PV, called the PV purity. To improve the PV purity while maintaining sufficient photon statistics, two PO selection criteria are introduced: the PO signal amplitude and the selection of POs uniquely associated with a pixel hit. The resulting increase in PV purity is 34 % for each selection criteria, while maintaining more than 20 POs for 98 % and 95 % of the PVs in the sample for the first and second selection respectively.| File | Dimensione | Formato | |
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