Status of the PandaRoot simulation of the Forward RICH

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Presentation transcript:

Status of the PandaRoot simulation of the Forward RICH Budker INP Status of the PandaRoot simulation of the Forward RICH Konstantin Beloborodov Budker INP, Novosibirsk, Russia Novosibirsk State University, Russia PANDA LIII. Collaboration Meeting Uppsala, Sweden 8-12 June 2015

Outline Geometry Aerogel Simulation Reconstruction

Forward RICH Dipole magnet RICH Main goal PID information for higher level triggers π/K-separation up to ~10 GeV/c Radiator Focusing aerogel Refractive indices ~1.05 Radiator thickness 4 cm Placement Between FT5 and FT6 Vertical angle ±5° Horizontal angle ±10° TOF HCAL FT5 FT6 RICH ECAL

Geometric requirements Placement along beam axis: between forward trackers 5 and 6 Angular acceptance: dimensions are the same or close to forward trackers dimensions Aerogel radiator: multi-layer Mirror: simple shape (flat, round, spheric) Geometric efficiency: all Cherenkov photons should be detected if it possible Photon detector: less sizes as it possible (due to cost optimization) Shape of Cherenkov “ring” on the photodetector surface: simple (circle, ellipse) … spheric round flat LHCb

Mirror parameters optimization Six segments flat mirror (as an example) Geometric efficiency: Lower Č photon hits PhDet Upper Č photon hits PhDet All other Č photons automatically do the same Photo detector width: w( z, l1, l2, l3, … ) → wmin First segment has major influence on PhDet size!

Optimal mirror configurations 1 segment 2 segments 3 segments 4 segments 6 segments 10 segments Round

Some features of flat and round mirrors 3 segments Round PD width, cm 67.5 58.5 Mirror focusing no yes Aerogel focusing combinatorial background Cherenkov “ring” shape on PD surface elliptical complicated Number of parts 3 1 round mirror Aerogel plate size = 60 cm (half height)

Multi-layer aerogel: parameter optimization Two layers Three layers 1.05 − δn 1.05 − δn 1.05 + δn 1.05 1.05 + δn Software: FairSoft – apr13, PandaRoot – scrut14

Multi-layer aerogel: optimal parameter Two layers Three layers n = 1.05 δnopt = 1.03·10-3 δnmin = 0.76·10-3 δnmax = 1.36·10-3 n = 1.05 δnopt = 1.23 ·10-3 δnmin = 0.96 ·10-3 δnmax = 1.47·10-3 Three segments mirror and three layer aerogel were used in further simulations

Events simulation and reconstruction Y, cm Reconstruction methods: on photodetector surface (template) photon track reconstruction (in order to obtain cherenkov angles for each hits) Y, cm θC, rad Y, cm X, cm X, cm θC = acos(1/n) X, cm φC, rad

Refraction on the surface of the aerogel θc, rad φc, rad θc = f( φc; β, n, α ) φc − azimuthal angle β − velocity of the charge particle n − refraction index of the aerogel α − polar angle of the charge particle

Fit result μ p = 10 GeV/c β = 0.99994 βFIT = 0.99912

Simulated effects Simulation Geometry description RICH position Aerogel (size, number of layers, refraction index) Mirror geometry (round, flat) Materials properties for Cherenkov photons Digitization Pixelation Quantum efficiency of photodetector Photodetector noise Dead time of photodetector Photodetector time resolution Crosstalks (not done) Reconstruction (simple mode) Hit preselection Fit θ(φ) dependence PID (not done) Probability calculation

Hit selection for fit 1000 events TA, ns θC, rad

π/K-separation: first result 2 GeV/c 4 GeV/c 6 GeV/c π π K K π K 8 GeV/c 10 GeV/c π K π K

Conclusions Geometry optimization for flat and round mirrors has been done Optimization of refractive indices for two and three layers aerogel has been performed First PANDAroot sim/digi/reco code for the Forward RICH has been created Events with single K and π mesons (FairBoxGenerator) going directlyto FRICH are simulated First and simple reconstruction of particle velocity has been realized First results on π/K separation has been obtained