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Separation of Cosmic-Ray Components in Water Cherenkov Detector

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Presentation on theme: "Separation of Cosmic-Ray Components in Water Cherenkov Detector"— Presentation transcript:

1 Separation of Cosmic-Ray Components in Water Cherenkov Detector
and use of neural networks to measure m/EM Luis Villaseñor* and H. Salazar FCFM-BUAP 5th International Workshop on Ring Imaging Cherenkov Detectors Playa del Carmen November 30 – December 5, 2004 *On Leave of Absence from IFM-UMSNH

2 Contents Motivation to study m/EM separation Experimental setup Data
Composition of showers with known m/EM Use of neural networks Conclusions

3 Nm/Ne Strongly Correlated With Primary Mass, i.e. ~2 x for Fe wrt p

4 Look here To understand there Use low energy data to get real
m and EM traces to eliminate systematics due to detector simulation Look here To understand there

5 Measure Charge, Amplitude,T10-50,T10-90
with good precision for three different triggers. Arbitrary muons threshold of 30mV

6 1.54 m diameter, 1.2 m water, one 8” PMT, tyvek 1/5 in volume of an Auger WCD

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8 LabView based DAS

9 ~74 pe

10 R shower (Q>7VEM) = 1 Hz
Low Charge Peak=0.12 VEM R muon = 876 Hz R EM = 80 Hz R shower (Q>7VEM) = 1 Hz Not an Artifact due to V threshold

11 Stopping muon at 0.1 VEM Decay electron at 0.18 VEM Crossing muon
Alarcón M. et al., NIM A 420 [1-2], 39-47 (1999).

12 Decay electron Stopping muon at 0.18 VEM at 0.1 VEM
In this case Qpeak=0.12 VEM EM particles of ~ 10 MeV Crossing muon at 1 VEM

13 With PMT Glass Cherenkov signal

14 No PMT Glass Cherenkov signal

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16 With PMT Glass Cherenkov signal

17 No PMT Glass Cherenkov signal

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21 Separation of individual Muons and EM particles is Easy for low energy Calibration events

22 Stopping muon or electron Q~0.12 VEM (9 pe) T12~3ns Isolated Muon
Shower Q>7 VEM (500 pe) T12>15ns

23 4 muons, 15ns Data trace Q=7.8 VEM 8 muons 15 ns 33 “electrons” 25 ns

24 Parameters for Data and Composed Events
Charge (VEM) Amplitude (V) T10-50 (ns) T10-90

25 2 or 3 classes as output (8m, 4m + 33e, 66e)
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)

26 Training and Clasification Results for Two Classes
8 m 4m 33 e Data 65% 39% 68% 35% 61% 32% Class

27 Training and Clasification Results for Two Classes
8 m 0m 66 e Data 65% 33% 78% 35% 67% 22% Class

28 Training and Clasification Results for Three Classes
8 m 0 e 4 m 33 e 0m 66 e Data 56% 29% 33% 58% 21% 35% 27% 15% 0 m 23% 36% 40% Class

29 Conclusions Clear separation of muons, electrons, PMT interactions 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: Apply to Auger with 25 ns sampling time.

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