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s ummer student se s s i on cern
Primary Vertex Reconstruction
for Upgrade at LHCb
Joanna Wanczyk under supervision of Agnieszka Dziurda
Joanna Wanczyk under supervision of Agnieszka Dziurda Primary Vertex Reconstructionfor Upgrade at LHCb 0 / 8
s ummer student se s s i on cern
My origins
Joanna Wanczyk under supervision of Agnieszka Dziurda Primary Vertex Reconstructionfor Upgrade at LHCb 1 / 8
s ummer student se s s i on cern
Upgrade LHCb Detector
Main changes
• Software and hardware trigger→ full software trigger
• VELO → VeloPix detector
• TT → Upstream Tracker
• T1-T3 stations → SciFidetector
nRecPV0 5 10 15 20
0
0.1
0.2
0.3
UpgradeRun II
LHCbunofficial
Running conditions
Energy [TeV ] Luminosity [cm−2s−1] Bunchspacing [ns] Data [fb−1]
Run I (2010-2012) 7/7/8 1/3.5/4 · 1032 50 3
Run II (2015-2018) 13 4 · 1032 25 5
Upgrade (>2020) 14 2 · 1033 25 50
Joanna Wanczyk under supervision of Agnieszka Dziurda Primary Vertex Reconstructionfor Upgrade at LHCb 2 / 8
s ummer student se s s i on cern
Definition
Position of the proton-proton collision inside the VELO (VErtex LOcator) detector at LHCbis obtained from the primary vertex reconstruction (PV) algorithms which use a set of inputtracks. In order to make the best performing reconstruction a wide range of parameters isbeing studied.
Joanna Wanczyk under supervision of Agnieszka Dziurda Primary Vertex Reconstructionfor Upgrade at LHCb 3 / 8
s ummer student se s s i on cern
Quality Parameters
dz 0.5− 0 0.5
0
5000
10000 LHCbunofficial
Figure 1 – The resolution for the zcoordinate in Run II.
dz 0.5− 0 0.5
0
100
200
300
400
310×
LHCbunofficial
Figure 2 – The resolution for the zcoordinate in Upgrade.
Definition
Resolution is defined as the differencebetween the fitted and generated position ofthe PV separately for each coordinate and isobtained as the averaged width of fitted tripleGaussian :
∆i = (iMC−ifit ) [mm], where i = {x, y , z}
Table 1 – The global resolution for the primaryvertex reconstruction.
Par. Run II Upgradeσx 0.013± 0.001 0.011± 0.001σz 0.075± 0.001 0.062± 0.001
Joanna Wanczyk under supervision of Agnieszka Dziurda Primary Vertex Reconstructionfor Upgrade at LHCb 4 / 8
s ummer student se s s i on cern
Quality Parameters
pseudo pull z 4− 2− 0 2 4
0
50
100
150310×
LHCbunofficial
Figure 3 – The pseudo pull for the zcoordinate in Upgrade.
pseudo pull z 4− 2− 0 2 4
0
2000
4000
LHCbunofficial
Figure 4 – The pseudo pull for the zcoordinate in Run II.
Definition
Pseudo pulls are calculated as a resolutiondivided by reconstructed position uncertainty :
pulli =∆i
σi, where i = {x, y , z}
Table 2 – The pseudo pulls for the primary vertexalgorithms.
Par. Run II Upgradeµx −0.007± 0.003 0.002± 0.002σx 1.031± 0.023 1.039± 0.005µz 0.032± 0.002 0.016± 0.001σz 1.017± 0.016 1.077± 0.004
Outcome
Good performance & stability
Joanna Wanczyk under supervision of Agnieszka Dziurda Primary Vertex Reconstructionfor Upgrade at LHCb 5 / 8
s ummer student se s s i on cern
Radial Distance Optimization
Definition
r distance is defined as :
r =√
(x1 − x2)2 + (y1 − y2)2
where (x2, y2) is PV position and (x1, y1) is the resolverposition which for MC is equal to (0, 0)
Purpose
Optimal value of rdistance must be foundin order to minimise thefalse PV efficiency andmaximise the true PVefficiency.
radial distance r [mm]0 0.05 0.1 0.15 0.2
0
0.05
0.1
Upgrade
Run II
LHCbunofficial
Figure 5 – Radial distance distributionsfor true PV.
radial distance r [mm]0 5 10 15
0
0.1
0.2
0.3
Upgrade
Run II
LHCbunofficial
Figure 6 – Radial distance distributionsfor false PV.
Joanna Wanczyk under supervision of Agnieszka Dziurda Primary Vertex Reconstructionfor Upgrade at LHCb 6 / 8
s ummer student se s s i on cern
Merits
FOM
The maximum of thepurity ∗ true PV efficiency sets the optimalvalue of r distance to r = 0.145 mm,where in Run II it was equalr = 0.18 mm for min bias sample.
radial distance r [mm]0 0.2 0.4 0.6 0.8 1
Eff
icie
ncy
(Pur
ity)
0.96
0.965
0.97
0.975
0.98
0.985
0.99
0.995
1
true PV efficiency
purity * true PV efficiency
(true + false) PVstrue PVspurity =
LHCbunofficial
Figure 7 – FOM for upgrade
Track multiplicity20 40 60 80 100 120 140
Eff
icie
ncy
0.4
0.5
0.6
0.7
0.8
0.9
1
=4nTracks
Upgrade, min
=4nTracks
Run II, minLHCbunofficial
Figure 8 – The PVs reconstruction efficiency as thefunction of track multiplicity
Efficiency
For the upgrade we have to be able to reconstructPVs consisting more tracks, although the totalefficiency of PV’s reconstruction for Upgradewhich equals 93.88% is comparable to the Run II is96.82%.
Joanna Wanczyk under supervision of Agnieszka Dziurda Primary Vertex Reconstructionfor Upgrade at LHCb 7 / 8
Thank you foryour attention !
Any Questions ?
s ummer student se s s i on cern
BACKUP
nTracks50 100 150
0
0.01
0.02
0.03
UpgradeRun II
LHCbunofficial
Figure 9 – Number of PVs per track multiplicity.
Joanna Wanczyk under supervision of Agnieszka Dziurda Primary Vertex Reconstructionfor Upgrade at LHCb 8 / 8