a c omparative study of the radiation hardness of plastic scintillators for the upgrade of the tile...
TRANSCRIPT
![Page 1: A C OMPARATIVE STUDY OF THE RADIATION HARDNESS OF PLASTIC SCINTILLATORS FOR THE UPGRADE OF THE TILE CALORIMETER OF THE ATLAS DETECTOR Shell-may Liao Supervisor:](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649d0a5503460f949dd1fb/html5/thumbnails/1.jpg)
1
A COMPARATIVE STUDY OF THE RADIATION HARDNESS OF PLASTIC SCINTILLATORS FOR THE UPGRADE OF THE TILE CALORIMETER OF THE
ATLAS DETECTOR
Shell-may Liao
Supervisor: Prof. Bruce Mellado
Thanks to: B. Mellado, E. Haddad, H. Jivan, C. Pelwan, G. Peters, iThemba LABS Gauteng team
![Page 2: A C OMPARATIVE STUDY OF THE RADIATION HARDNESS OF PLASTIC SCINTILLATORS FOR THE UPGRADE OF THE TILE CALORIMETER OF THE ATLAS DETECTOR Shell-may Liao Supervisor:](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649d0a5503460f949dd1fb/html5/thumbnails/2.jpg)
2
OUTLINE
Introduction Scintillation mechanism SRIM and TRIM simulations Sample preparation Radiation process Transmission spectroscopy Results and analysis Conclusion
![Page 3: A C OMPARATIVE STUDY OF THE RADIATION HARDNESS OF PLASTIC SCINTILLATORS FOR THE UPGRADE OF THE TILE CALORIMETER OF THE ATLAS DETECTOR Shell-may Liao Supervisor:](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649d0a5503460f949dd1fb/html5/thumbnails/3.jpg)
3
INTRODUCTION
Main problem encountered by scintillators
Scintillators exhibit luminescence when excited by ionizing radiation
PVT based scintillators: EJ 200, EJ 208, EJ 260
Experimental procedure sample dimensions: 500μm x 500μm x 350 μm
![Page 4: A C OMPARATIVE STUDY OF THE RADIATION HARDNESS OF PLASTIC SCINTILLATORS FOR THE UPGRADE OF THE TILE CALORIMETER OF THE ATLAS DETECTOR Shell-may Liao Supervisor:](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649d0a5503460f949dd1fb/html5/thumbnails/4.jpg)
4
SCINTILLATION MECHANISM
Common feature in plastic scintillator = benzene ring
Delocalized electrons are prone to excitation
Electronic levels of a PVT molecule
PVT base is doped with flours
Fluors absorb the base scintillation and emit at longer wavelengths
![Page 5: A C OMPARATIVE STUDY OF THE RADIATION HARDNESS OF PLASTIC SCINTILLATORS FOR THE UPGRADE OF THE TILE CALORIMETER OF THE ATLAS DETECTOR Shell-may Liao Supervisor:](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649d0a5503460f949dd1fb/html5/thumbnails/5.jpg)
5
SRIM SIMULATIONS
About SRIM
Stopping Range of 6MeV protons in PVT
Stopping range = 474.17 μm
![Page 6: A C OMPARATIVE STUDY OF THE RADIATION HARDNESS OF PLASTIC SCINTILLATORS FOR THE UPGRADE OF THE TILE CALORIMETER OF THE ATLAS DETECTOR Shell-may Liao Supervisor:](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649d0a5503460f949dd1fb/html5/thumbnails/6.jpg)
6
TRIM SIMULATIONS
Transport of 6MeV protons in PVT
Average energy of transmitted protons = 2.8MeV
Thus energy lost by 6MeV protons = 3.2MeV
![Page 7: A C OMPARATIVE STUDY OF THE RADIATION HARDNESS OF PLASTIC SCINTILLATORS FOR THE UPGRADE OF THE TILE CALORIMETER OF THE ATLAS DETECTOR Shell-may Liao Supervisor:](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649d0a5503460f949dd1fb/html5/thumbnails/7.jpg)
7
SAMPLE PREPARATION Employed metallographic techniques:
• Documentation• 20 cm x 2 cm x
1cm• Sectioning and
cutting• Mounting• Rough Polishing• Final polishing
Polished samples range:
300 μm – 380 μm
![Page 8: A C OMPARATIVE STUDY OF THE RADIATION HARDNESS OF PLASTIC SCINTILLATORS FOR THE UPGRADE OF THE TILE CALORIMETER OF THE ATLAS DETECTOR Shell-may Liao Supervisor:](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649d0a5503460f949dd1fb/html5/thumbnails/8.jpg)
8
RADIATION PROCESS
Tandem accelerator of iThemba LABS Gauteng
Exposure doses:• 80 MGy• 25 MGy• 8 MGy• 0.8 MGy
![Page 9: A C OMPARATIVE STUDY OF THE RADIATION HARDNESS OF PLASTIC SCINTILLATORS FOR THE UPGRADE OF THE TILE CALORIMETER OF THE ATLAS DETECTOR Shell-may Liao Supervisor:](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649d0a5503460f949dd1fb/html5/thumbnails/9.jpg)
9
RADIATION PROCESS
![Page 10: A C OMPARATIVE STUDY OF THE RADIATION HARDNESS OF PLASTIC SCINTILLATORS FOR THE UPGRADE OF THE TILE CALORIMETER OF THE ATLAS DETECTOR Shell-may Liao Supervisor:](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649d0a5503460f949dd1fb/html5/thumbnails/10.jpg)
10
TRANSMISSION SPECTROSCOPY
Why transmission spectroscopy?
Dual beam spectrometer
Spectra recorded as percentage of light transmission through air
![Page 11: A C OMPARATIVE STUDY OF THE RADIATION HARDNESS OF PLASTIC SCINTILLATORS FOR THE UPGRADE OF THE TILE CALORIMETER OF THE ATLAS DETECTOR Shell-may Liao Supervisor:](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649d0a5503460f949dd1fb/html5/thumbnails/11.jpg)
11
TRANSMISSION SPECTROSCOPY
![Page 12: A C OMPARATIVE STUDY OF THE RADIATION HARDNESS OF PLASTIC SCINTILLATORS FOR THE UPGRADE OF THE TILE CALORIMETER OF THE ATLAS DETECTOR Shell-may Liao Supervisor:](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649d0a5503460f949dd1fb/html5/thumbnails/12.jpg)
12
UNIRRADIATED TRANSMISSION DATA
EJ 200 – 85.7%
EJ 208 – 83.2%
EJ 260 – 80.8%
![Page 13: A C OMPARATIVE STUDY OF THE RADIATION HARDNESS OF PLASTIC SCINTILLATORS FOR THE UPGRADE OF THE TILE CALORIMETER OF THE ATLAS DETECTOR Shell-may Liao Supervisor:](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649d0a5503460f949dd1fb/html5/thumbnails/13.jpg)
13
EJ 208 & EJ 260 TRANSMISSION PLOTS
![Page 14: A C OMPARATIVE STUDY OF THE RADIATION HARDNESS OF PLASTIC SCINTILLATORS FOR THE UPGRADE OF THE TILE CALORIMETER OF THE ATLAS DETECTOR Shell-may Liao Supervisor:](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649d0a5503460f949dd1fb/html5/thumbnails/14.jpg)
14
TRANSMISSION DATA
![Page 15: A C OMPARATIVE STUDY OF THE RADIATION HARDNESS OF PLASTIC SCINTILLATORS FOR THE UPGRADE OF THE TILE CALORIMETER OF THE ATLAS DETECTOR Shell-may Liao Supervisor:](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649d0a5503460f949dd1fb/html5/thumbnails/15.jpg)
15
EJ 208 TRANSMISSION PLOT (ANNEALING ID)
![Page 16: A C OMPARATIVE STUDY OF THE RADIATION HARDNESS OF PLASTIC SCINTILLATORS FOR THE UPGRADE OF THE TILE CALORIMETER OF THE ATLAS DETECTOR Shell-may Liao Supervisor:](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649d0a5503460f949dd1fb/html5/thumbnails/16.jpg)
16
EJ 200 TRANSMISSION PLOT (ANNEALING ID)
![Page 17: A C OMPARATIVE STUDY OF THE RADIATION HARDNESS OF PLASTIC SCINTILLATORS FOR THE UPGRADE OF THE TILE CALORIMETER OF THE ATLAS DETECTOR Shell-may Liao Supervisor:](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649d0a5503460f949dd1fb/html5/thumbnails/17.jpg)
17
CONCLUSION Radiation exposure = decrease in light transmission in all
grades
Increase in dose = decrease in transmission
Samples undergo annealing
Possible formation of free radicals (EPR)
Raman and light yield studies were done by Ms. Harshna Jivan
EJ 208 exhibits the best light transmission properties Lowest decrease in % transmission for most doses Large amount of healing in short period of time.
![Page 18: A C OMPARATIVE STUDY OF THE RADIATION HARDNESS OF PLASTIC SCINTILLATORS FOR THE UPGRADE OF THE TILE CALORIMETER OF THE ATLAS DETECTOR Shell-may Liao Supervisor:](https://reader035.vdocuments.mx/reader035/viewer/2022062421/56649d0a5503460f949dd1fb/html5/thumbnails/18.jpg)
18
According to Markley et al, “A radiation hard plastic scintillator can be defined as a
scintillator that does not exhibit a large decrease in light yield output when exposed to ionizing radiation and which can recover a
substantial amount of its light output in a short time after being irradiated”.