particle identification in ecal
DESCRIPTION
Particle identification in ECAL. Yuri Kharlov, Alexander Artamonov IHEP, Protvino CBM collaboration meeting 28.09.2007. PID methods applicable for ECAL. The aim of ECAL PID is to discriminate and e from anything else Charged track matching - PowerPoint PPT PresentationTRANSCRIPT
![Page 1: Particle identification in ECAL](https://reader035.vdocuments.site/reader035/viewer/2022062408/5681386a550346895da01986/html5/thumbnails/1.jpg)
28.09.2007 ECAL PID 1
Particle identification in ECAL
Yuri Kharlov, Alexander ArtamonovIHEP, Protvino
CBM collaboration meeting28.09.2007
![Page 2: Particle identification in ECAL](https://reader035.vdocuments.site/reader035/viewer/2022062408/5681386a550346895da01986/html5/thumbnails/2.jpg)
28.09.2007 ECAL PID 2
PID methods applicable for ECAL
The aim of ECAL PID is to discriminate and e from anything else
• Charged track matching– Reject (for ) or identify (for e) ECAL clusters produced by
charged tracks
• Flight time measurement– Reject ECAL clusters produced by slow particles (mainly heavy
hadrons)
• Transverse shower shape– Discriminate electromagnetic and hadronic showers
• Longitudinal shower profile– Discriminate electromagnetic and hadronic showers
![Page 3: Particle identification in ECAL](https://reader035.vdocuments.site/reader035/viewer/2022062408/5681386a550346895da01986/html5/thumbnails/3.jpg)
28.09.2007 ECAL PID 3
Flight time from target to ECAL (12 m)
Neutral hadrons contribute to photon spectrum mainly at E<2 GeV
Significant background is expected from antineutrons at 1.8 GeV
Time resolution t=1 ns is sufficient for rejection of K0 and neutrons
![Page 4: Particle identification in ECAL](https://reader035.vdocuments.site/reader035/viewer/2022062408/5681386a550346895da01986/html5/thumbnails/4.jpg)
28.09.2007 ECAL PID 4
Longitudinal profile of electromagnetic shower (PDG)
![Page 5: Particle identification in ECAL](https://reader035.vdocuments.site/reader035/viewer/2022062408/5681386a550346895da01986/html5/thumbnails/5.jpg)
28.09.2007 ECAL PID 5
Prototype of “Two-Sections” ECAL Module
Two channel PMT based on PM FEU-
115M dynode system
110
450
20X0 = 10X0 + 10X0
Total radiation length = 20Xo.Number of layers = 85Lead plate thickness = 1.3 mmScintillator plate thickness = 4.0 mmScintillator – Polystyrene + 1.5%PT + 0.05% POPOPWave Length Shifting Fibers – Y11
Lucite prism for uniform light
mixing
Light from the first half of calorimeter (preshower) was collected to one anode and light from the second half to another.
V.Brekhovskikh, V.Rykalin 21 September 2006
![Page 6: Particle identification in ECAL](https://reader035.vdocuments.site/reader035/viewer/2022062408/5681386a550346895da01986/html5/thumbnails/6.jpg)
28.09.2007 ECAL PID 6
2-segment module designSeparate light collection to 2-channel PMT
V.Brekhovskikh, V.Rykalin 21 September 2006
![Page 7: Particle identification in ECAL](https://reader035.vdocuments.site/reader035/viewer/2022062408/5681386a550346895da01986/html5/thumbnails/7.jpg)
28.09.2007 ECAL PID 7
All
calo
rim
ete
r
Preshower
Accepted electrons (84%)
Rejected pions (93%)
Beam measurements of 2-segment module
V.Brekhovskikh, V.Rykalin 21 September 2006
![Page 8: Particle identification in ECAL](https://reader035.vdocuments.site/reader035/viewer/2022062408/5681386a550346895da01986/html5/thumbnails/8.jpg)
28.09.2007 ECAL PID 8
Simulation model
• 1 module with 160 layers (Pb 0.7 mm + Sci 1.0 mm)
• Total radiation length: 20X0.
• 20 longitudinal segments, each of 8 layers
• Various combinations of energies deposited in different segments allow to optimize longitudinal segmentation
![Page 9: Particle identification in ECAL](https://reader035.vdocuments.site/reader035/viewer/2022062408/5681386a550346895da01986/html5/thumbnails/9.jpg)
28.09.2007 ECAL PID 9
Edet vs Segment number: 5 GeV
Photons Hadrons
![Page 10: Particle identification in ECAL](https://reader035.vdocuments.site/reader035/viewer/2022062408/5681386a550346895da01986/html5/thumbnails/10.jpg)
28.09.2007 ECAL PID 10
Edet vs Segment number : 10 GeV
Photons Hadrons
![Page 11: Particle identification in ECAL](https://reader035.vdocuments.site/reader035/viewer/2022062408/5681386a550346895da01986/html5/thumbnails/11.jpg)
28.09.2007 ECAL PID 11
Edet vs Segment number : 15 GeV
Photons Hadrons
![Page 12: Particle identification in ECAL](https://reader035.vdocuments.site/reader035/viewer/2022062408/5681386a550346895da01986/html5/thumbnails/12.jpg)
28.09.2007 ECAL PID 12
Longitudinal profile: Photons
5 GeV 10 GeV
![Page 13: Particle identification in ECAL](https://reader035.vdocuments.site/reader035/viewer/2022062408/5681386a550346895da01986/html5/thumbnails/13.jpg)
28.09.2007 ECAL PID 13
Longitudinal profile: Hadrons
5 GeV 10 GeV
![Page 14: Particle identification in ECAL](https://reader035.vdocuments.site/reader035/viewer/2022062408/5681386a550346895da01986/html5/thumbnails/14.jpg)
28.09.2007 ECAL PID 14
Longitudinal profile: Muons
5 GeV 10 GeV
![Page 15: Particle identification in ECAL](https://reader035.vdocuments.site/reader035/viewer/2022062408/5681386a550346895da01986/html5/thumbnails/15.jpg)
28.09.2007 ECAL PID 15
E1/E2, 5 GeV (1X0+19X0)
![Page 16: Particle identification in ECAL](https://reader035.vdocuments.site/reader035/viewer/2022062408/5681386a550346895da01986/html5/thumbnails/16.jpg)
28.09.2007 ECAL PID 16
E1/E2, 5 GeV (2X0+18X0)
![Page 17: Particle identification in ECAL](https://reader035.vdocuments.site/reader035/viewer/2022062408/5681386a550346895da01986/html5/thumbnails/17.jpg)
28.09.2007 ECAL PID 17
E1/E2, 5 GeV (3X0+17X0)
![Page 18: Particle identification in ECAL](https://reader035.vdocuments.site/reader035/viewer/2022062408/5681386a550346895da01986/html5/thumbnails/18.jpg)
28.09.2007 ECAL PID 18
E1/E2, 5 GeV (4X0+16X0)
![Page 19: Particle identification in ECAL](https://reader035.vdocuments.site/reader035/viewer/2022062408/5681386a550346895da01986/html5/thumbnails/19.jpg)
28.09.2007 ECAL PID 19
Identification probabilities (1X0+19X0)
E1/E2 cut
0.005 0.010 0.015 0.020 0.025 0.030
5 GeV 0.725 0.872 0.938 0.962 0.969 0.972
- 0.200 0.331 0.381 0.405 0.424 0.447
10 GeV 0.857 0.957 0.968 0.970 0.970 0.970
- 0.250 0.357 0.405 0.439 0.462 0.482
15 GeV 0.925 0.970 0.972 0.972 0.972 0.972
- 0.281 0.381 0.425 0.451 0.474 0.498
S/B=3.5
![Page 20: Particle identification in ECAL](https://reader035.vdocuments.site/reader035/viewer/2022062408/5681386a550346895da01986/html5/thumbnails/20.jpg)
28.09.2007 ECAL PID 20
Identification probabilities (2X0+18X0)
E1/E2 cut
0.010 0.030 0.035 0.045 0.055 0.065
5 GeV 0.418 0.563 0.734 0.821 0.882 0.920
- 0.132 0.287 0.366 0.389 0.406 0.426
10 GeV 0.525 0.716 0.886 0.940 0.960 0.967
- 0.196 0.318 0.394 0.421 0.442 0.463
15 GeV 0.608 0.818 0.948 0.966 0.970 0.972
- 0.229 0.346 0.414 0.436 0.455 0.476
S/B=3
![Page 21: Particle identification in ECAL](https://reader035.vdocuments.site/reader035/viewer/2022062408/5681386a550346895da01986/html5/thumbnails/21.jpg)
28.09.2007 ECAL PID 21
Identification probabilities (3X0+17X0)E1/E2
cut0.05 0.10 0.15 0.20 0.25
5 GeV 0.432 0.689 0.865 0.938 0.965
- 0.330 0.395 0.550 0.774 0.840
10 GeV 0.582 0.867 0.955 0.969 0.970
- 0.359 0.436 0.596 0.835 0.907
15 GeV 0.692 0.939 0.970 0.972 0.972
- 0.381 0.445 0.612 0.857 0.924
S/B=2
![Page 22: Particle identification in ECAL](https://reader035.vdocuments.site/reader035/viewer/2022062408/5681386a550346895da01986/html5/thumbnails/22.jpg)
28.09.2007 ECAL PID 22
Identification probabilities (4X0+16X0)
E1/E2 cut
0.10 0.20 0.30 0.40 0.50
5 GeV 0.334 0.613 0.824 0.925 0.960
- 0.341 0.462 0.775 0.835 0.853
10 GeV 0.466 0.810 0.943 0.967 0.970
- 0.380 0.517 0.849 0.916 0.935
15 GeV 0.576 0.906 0.967 0.972 0.972
- 0.394 0.530 0.866 0.933 0.952
S/B=1.5
![Page 23: Particle identification in ECAL](https://reader035.vdocuments.site/reader035/viewer/2022062408/5681386a550346895da01986/html5/thumbnails/23.jpg)
28.09.2007 ECAL PID 23
To do
• 3-segment module: the optimal segmentation to be found• Realistic momentum distribution of incoming particles• Realistic particle multiplicity to be studied• Track-ECAL matching and optimization of the matching
distance for charged particle rejection• Simulation of realistic TOF measurement in ECAL and
optimization of ECAL-TOF cut for heavy hadron rejection• Photon identification efficiency and hadron contamination
of the photon spectrum in central HI collisions