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Construct two layers of hadron calorimeter and test Makoto Harada High Energy Physics Laboratory Faculty of Physics Department of Science Shinshu University.

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Presentation on theme: "Construct two layers of hadron calorimeter and test Makoto Harada High Energy Physics Laboratory Faculty of Physics Department of Science Shinshu University."— Presentation transcript:

1 Construct two layers of hadron calorimeter and test Makoto Harada High Energy Physics Laboratory Faculty of Physics Department of Science Shinshu University

2 The purpose of this study I constructed two layers of hadron calorimeter and tried to detect point where cosmic rays passed. I tested my hadron calorimeter by using Geant4 simulation. Improve detection accuracy and energy resolution of ILD hadron calorimeter

3 Hadron calorimeter A detector which causes hadron shower to hadron and measures its energy. total track length of all generated particles measuring total track length → measuring incidence particle energy It is essential to detect the point where a particle passed accurately. incidence particle energy

4 Two layers of hadron calorimeter A particle Absorber : Tungsten alloy (Thickness 3.5 mm ) Gap : Scintillators (Thickness 2.0 mm ) Scintillators are divided into 18 bars. Scintillator bars of 1st and 2nd layer are orthogonal. A particle (point passed by a particle) These two scintillators radiate light. A particle passed common square area of these two scintillators.

5 ReflectorScintillator ・ prevent light from escaping out of scintillators ・ get independent signal from each scintillators → wrap each scintillators in a reflector I made 36 scintillators wrapped in a reflector Scintillation light using fiber no fiber gathered by wave length shift fiber detected by MPPC MPPC ・・・ a new type of photodetector ・ small size and reasonable price ・ photocounting efficiency ・ tolerance to magnetic field MPPC Constructing hadron calorimeter Absorber side Gap side Structure of absorber is tungsten alloy plates Structure of gap is 18 scintillators

6 magnification ADC distribution of MPPC (use ) Count of events ADC Count : the difference between peak and peak Average Photo Electron ( ) → divided into the average of ADC count more than 36 scintillators efficiency test (use ) Average Photo Electron (p.e.) Scintillator number Average : Standard deviation : No.1 ~ 18 scintillator → 1st layer No.19 ~ 36 scintillator → 2nd layer

7 I detected scintillation light using MPPCs. Then, I made ADC distribution about each MPPCs. two layers of hadron calorimeter I set two PMTs up and down hadron calorimeter and used them as trigger. Scintillator of trigger 1 Scintillator of trigger 2 Experiment with cosmic raysTwo layers of hadron calorimeter A side view

8 The relation between trigger scintillators and hadron calorimeter ①②③④⑤⑥⑦⑧⑨⑩⑪⑫⑬⑭⑮⑯⑰⑱ ① ② ③ ④ ⑤ ⑥ ⑦ ⑧ ⑨ ⑩ ⑪ ⑫ ⑬ ⑭ ⑮ ⑯ ⑰ ⑱ 1st layer 2nd layer Trigger 1 Trigger 2 When cosmic rays pass this common area, the ADC gate is opened. ⑩⑪⑫⑬⑭⑮⑯⑰⑱ ⑩ ⑪ ⑫ ⑬ ⑭ ⑮ ⑯ ⑰ ⑱ ① ②③④⑤⑥⑦⑧⑨ ① ② ④ ⑤ ⑥ ⑦ ⑧ ⑨ ③ I can get data from No.1 ~ 9 scintilator of each layers. 2nd layer 1st layer

9 Curtain box Circuit diagram

10 Results of experiment I measured cosmic rays 20000 times. I changed ADC count into photo electron. 1st layer 1st2nd3rd4th 5th 6th7th8th9th This is an example of one of the events. This data shows point where a cosmic ray passed. 2nd layer

11 P.E. distribution P.E. distribution (Landau fit) the peak of Landau fit : Count of events

12 Sum of events about scintillators of 2nd layer Sum of events about scintillators of 1st layer Histogram of point passed by cosmic rays Detection rate : Scintillator number of 2nd layer Scintillator number of 1st layer Count of events

13 Geant4 simulation Hadron calorimeter planned to be used in ILD ・ Absorber : Pure iron ( Thickness,Density ) ・ Gap : Scintillator ( Thickness ) ・ Number of layers : ・ Size : ( To compare my hadron calorimeter ) I researched energy resolution through simulation that shoots, and particles for this hadron calorimeter.

14 Results of simulation I require my hadron calorimeter to satisfy this resolution I research how many layers will need by using Genat4 simulation. Energy Resolution

15 My Hcal : 100 layers Comparing resolution ILD Hcal : 48 layers absorber : pure iron ( thickness ) gap : scintillator (thickness ) Energy Resolution Energy Resolution absorber : tungsten alloy ( thickness ) gap : scintillator (thickness )

16 Conclusion My hadron calorimeter needs 100 layers to satisfy energy resolution of ILD hadron calorimeter. ( thickness of hadron calorimeter will be half ) Using cross scintillators, I succeeded in detecting the point where cosmic rays had passed. My hadron calorimeter showed 7 photo electron. I constructed two layers of hadron calorimeter.

17 Tasks I Investigate how much photo electron increases by using Scintillators which are in thickness. I make a histogram of point passed by particles through simulation that shoots them for hadron calorimeter whose each gap are divided into 18 bars.


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