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Measurement of momentum for charged particles Detector Basic 18/07/18 M2 Yosuke Kobayashi Measurement of momentum Charged particle traveling in a magnetic field is acted on Lorentz force. : charge = :


  1. Measurement of momentum for charged particles Detector Basic 18/07/18 M2 Yosuke Kobayashi

  2. Measurement of momentum β€’ Charged particle traveling in a magnetic field is acted on Lorentz force. π‘Ÿ : charge 𝑔 = π‘Ÿπ’˜ Γ— π‘ͺ 𝐢 : magnetic field strength 𝑀 : velocity β€’ If the strength of the magnetic field and the radius are known, the momentum can be measured. B e + 𝑛𝑀 π‘ž 𝑠 = π‘ŸπΆ = π‘ŸπΆ r 𝑛 : mass of particle π‘ž [π»π‘“π‘Š/𝑑] = 0.3 𝑠 𝑛 𝐢[π‘ˆ] 2

  3. Measurement method β€’ Tracks are reconstructed by each detector. - The momentum is determined from the radius and the charge is obtained from the direction of bending. β€’ Track reconstruction detectors - Gas multiplication detector - Position resolution : 50 ~ 300 ΞΌm - Scintillation counter - Position resolution : Different by scintillator… - Semiconductor detector - Position resolution : Different by pixel size… 3

  4. Real application β€’ The measured track is close a straight line in real application. β€’ sagitta s is calculated. 2 𝑠 2 = (𝑠 βˆ’ 𝑑) 2 + 𝑀 s 2 L r-s 𝑠 2 βˆ’ 𝑀 2 r 𝑑 = 𝑠 βˆ’ 4 B 2 + 𝑀 2 8𝑑 β‰ˆ 𝑀 2 𝑠 = 𝑑 8𝑑 (𝑑 β‰ͺ 𝑀) The relation between radius and momentum π‘ŸπΆ ⟹ 𝑑 = π‘ŸπΆπ‘€ 2 𝑠 = π‘ž π‘ž 4

  5. β€’ Reference β€’ http://summerstudents.desy.de/e69118/e177730/e2 02573/Detectors_Summer2015_part4.pdf 5

  6. Appendix π‘ž = 𝑛𝑀 = π‘ π‘ŸπΆ [kg ・ m/s] 𝑠 : radius [m] π‘Ÿ : charge π‘žπ‘‘ = π‘ π‘ŸπΆπ‘‘ [J] 𝐢 : magnetic field strength [T] π‘ π‘ŸπΆπ‘‘ 1.6Γ—10 βˆ’19 [eV] π‘žπ‘‘ = π‘žπ‘‘ = 𝑠𝐢𝑑 [eV] π‘žπ‘‘ = 𝑠𝐢 βˆ™ 3.0 Γ— 10 8 [eV] π‘ž = 0.3𝑠𝐢 [GeV/c] 6

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