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DE/dx Study at CEPC TPC An Fenfen 2017.02.28.

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Presentation on theme: "DE/dx Study at CEPC TPC An Fenfen 2017.02.28."β€” Presentation transcript:

1 dE/dx Study at CEPC TPC An Fenfen

2 dE/dx Meas. @ TPC And, momentum and cosπœƒ of the incident particle
𝑁 π‘π‘Žπ‘‘ : number of pad circles β„Ž π‘π‘Žπ‘‘ : pad size in the radial direction Gas density (atmosphere pressure, temperature, gas type) a large vessel contains an ionisable gas (mixture of Argon and methane) in which charged particles produce ionization electrons. An electric field lets these electrons drift in the vessel towards a MWPC located at the end of the drift volume. Endcap is Micropattern Gaseous Detectors. Magnetic field parrellel to E, to focus the electrons. And, momentum and cosπœƒ of the incident particle (πœƒ is the angle between the particle and z axis)

3 Space Charge Effect s s 𝒉 𝒑𝒂𝒅 𝒉 𝒑𝒂𝒅 ΞΈ ΞΈ
π‘β„Žπ‘Žπ‘Ÿπ‘”π‘’ 𝑑𝑒𝑛𝑠𝑖𝑑𝑦= 𝑑𝐸 𝑑π‘₯ βˆ— 𝑠 β„Ž π‘π‘Žπ‘‘ = 𝑑𝐸 𝑑π‘₯ β‹… 1 sinΞΈ Smaller πœƒβ†’ Larger charger density s s 𝒉 𝒑𝒂𝒅 𝒉 𝒑𝒂𝒅 ΞΈ ΞΈ 𝜎 𝑑𝐸/𝑑π‘₯ = 2.53βˆ’0.77 π‘π‘œπ‘ πœƒ π‘π‘œπ‘ πœƒ 10 𝑡 𝒑𝒂𝒅 𝐝𝐞𝐜𝐫𝐞𝐚𝐬𝐞𝐬 when track is parallel to Z

4 New 5-d Formula Based on G4
𝜎 𝑑𝐸/𝑑π‘₯ πœ‡ 𝑑𝐸/𝑑π‘₯ = 𝑁 π‘π‘Žπ‘‘ βˆ— (β„Ž π‘π‘Žπ‘‘ β‹…πœŒ) 𝑒 βˆ’0.1𝑝 (2.53βˆ’0.77 π‘π‘œπ‘ πœƒ π‘π‘œπ‘ πœƒ 10 ) 𝑁 π‘π‘Žπ‘‘ : β„Ž π‘π‘Žπ‘‘ (mm): 1-35 𝜌(mg/cm3): 0.16~2(1-10atm) 𝑝(GeV/c): 1-100 For He-based gas with a large fraction of hydrocarbon, the power in (β„Ž π‘π‘Žπ‘‘ β‹…πœŒ) 0.3 should be changed to (β„Ž π‘π‘Žπ‘‘ β‹…πœŒ) 0.45 𝜎 𝑑𝐸/𝑑π‘₯ πœ‡ 𝑑𝐸/𝑑π‘₯ = 𝑁 π‘π‘Žπ‘‘ βˆ— (β„Ž π‘π‘Žπ‘‘ β‹…πœŒ) 𝑒 βˆ’0.1𝑝 (2.53βˆ’0.77 π‘π‘œπ‘ πœƒ π‘π‘œπ‘ πœƒ 10 )

5 Gas Type In order to separate the two groups with(out) much hydrocarbon, the normalization factor is different

6 𝜎/πœ‡~ (Δ𝑅, 𝑁 π‘π‘Žπ‘‘ )

7 Comparison With Other Exp.

8 Comparison With Other Exp.

9 Truncation In dE/dx Calculation
We measure the average dE/dx value of one track by removing parts of its hits (noise and Landau tail) For 20GeV πœ‹ with direction (0,1,1) in default geometry, 𝜎/πœ‡ with different truncation: 0-1: 2.64 0-0.95: 2.24 0-0.9: 2.22 0-0.8: 2.28 0-0.65: 2.43 : 2.31 Loss of 30% hits will increase the resolution by ~4%

10 πœ‡ 𝑑𝐸/𝑑π‘₯ ~ 𝛽𝛾 E 𝑐𝑒𝑑 =851eV, determined by fitting the G4 plots
πœ‡ 𝑑𝐸/𝑑π‘₯ ~ 𝛽𝛾 E 𝑐𝑒𝑑 =851eV, determined by fitting the G4 plots , 𝑬 𝒄𝒖𝒕 =851eV (fit par.)

11 dE/dx For Different Particles
𝜎 πœ‡ ~𝑝 πœ‡~𝑝 πœ‡ 1 βˆ’ πœ‡ 𝜎 𝜎 2 2 Definition of separation ability:

12 Separation Ability 2.4𝝈~πŸ’.πŸ“% π’Žπ’Šπ’” π’Šπ’… 3.9𝝈~𝟎.πŸ‘% π’Žπ’Šπ’” π’Šπ’…
Entrance angle (0,1,1) 2.4𝝈~πŸ’.πŸ“% π’Žπ’Šπ’” π’Šπ’… 3.9𝝈~𝟎.πŸ‘% π’Žπ’Šπ’” π’Šπ’… Dash-dotted line corresponds to the case I doubled the 𝜎/πœ‡

13 Summary & Outlook Geant4 prediction would be lower than the experimental measurement, but double the G4 value would be safe. Preliminary result of the separation ability is given.

14 A Screenshot From INFN Report
Dash-dotted line corresponds to the case using clustering counting techneque

15 Comparison With Other Exp.


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