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“Separation of cosmic-ray components in a single water Cherenkov detector"

“Separation of cosmic-ray components in a single water Cherenkov detector". Yasser Jerónimo, Luis Villaseñor IFM-UMSNH. H. Salazar FCFM-BUAP. X Mexican School of Particles and Fields Playa del Carmen November 5, 2002. Contents. Celebration in Honor of Augusto and Arnulfo

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“Separation of cosmic-ray components in a single water Cherenkov detector"

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  1. “Separation of cosmic-ray components in a single water Cherenkov detector" Yasser Jerónimo, Luis Villaseñor IFM-UMSNH H. Salazar FCFM-BUAP X Mexican School of Particles and Fields Playa del Carmen November 5, 2002

  2. Contents • Celebration in Honor of Augusto and Arnulfo • Arnulfo and Auger • Motivation to study m/EM separation • Experimental setup • Data • Composition of showers with known m/EM • Use of neural networks • Conclusions

  3. THE MEXICAN GROUP R. López

  4. Objectives • Take part in a major UHE cosmic ray project • Graduate students • Popularize physics of cosmic rays • Motivate and involve Mexican industry in the project R.López

  5. Participants R. López

  6. Students Graduated ~6 refereed papers, ~60 in proceedings and ~200 talks for general public R. López

  7. Activities in Mexico Water Cherenkov detectors in Puebla and Morelia (ICFA Instrumentation Center), Calibration, Schmidt Optics, Simulation, Theory, Data Analysis.

  8. Industry Rotomolded Polyethylene Tanks R.López

  9. Use low energy showers to study m-EM separation Look here To understand over there

  10. 1.54 m diameter, 1.2 m water, 1 8” PMT, tyvek 1/5 in volume of an Auger WCD

  11. 2GS/s vs 40MS/s ns for Auger

  12. Stopping muon at 0.1 VEM Decay electron at 0.18 VEM Crossing muon at 1 VEM Alcaraz et al., NIM 2000

  13. Measure Charge, Amplitude,T10-50,T10-90 with good precision

  14. LabView based DAS

  15. Three types of triggers Vertical muons

  16. ~74 pe

  17. Arbitrary muons Threshold of 30mV

  18. Low Charge Peak=0.12 VEM Stopping muons and eletrons R muon=876 Hz R sm+e=80 Hz R shower (Q>7VEM)=1 Hz Not an Artifact due to V threshold

  19. Decay electron at 0.18 VEM Stopping muon at 0.1 VEM Qpeak=0.12 VEM Stopping Muon or electron of ~30MeV Crossing muon at 1 VEM

  20. No PMT Glass Cherenkov signal

  21. With PMT Glass Cherenkov signal

  22. Charge Distributions for Crossing and stopping muons around 1 and .12VEM Stopping muons and eletrons

  23. No PMT Glass Cherenkov signal

  24. With PMT Glass Cherenkov signal

  25. Stopping muons and eletrons

  26. Stopping muons and eletrons Single Muons

  27. Separation of individual Muons and Stopping muons or electrons possible Single Muons Stopping muons and elctrons

  28. Stopping muon or electron Q~0.12 VEM T12~3ns Isolated Muon Q~1 VEM T12~12 ns Shower Q>7 VEM T12>15ns

  29. Data trace Q=7.8 VEM 8 muons 15 ns 4 muons, 15ns 33 “electrons” 25 ns 66 “electrons” 25 ns

  30. Parameters for Data and Composed Events

  31. Training and Clasification Results for a Kohonen Neural Network 4 features as input (Charge, Amplitude, T10-50, T1090) 8 Neurons in first layer 4 in second layer 2 or 3 classes as output (8m, 4m + 33e, 66e)

  32. Training and Clasification Results for Two Classes Class

  33. Training and Clasification Results for Two Classes Class

  34. Training and Clasification Results for Three Classes Class

  35. Conclusions Clear separation of crossing muons, PMT interactions, stopping muons and showers in a single WCD Rise time 10-50% is linear with Q/V Neural Networks classify composed events of muons and “electrons” better than randomly Shower data is dominated by muons To do: use real electron pulses from m decay and other features like power spectrum distribution. Use wider Auger showers (ms) with 25 ns sampling time.

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