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Development of a Liquid Scintillator and of Data ... - Borexino - Infn

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5 Particle Identification with a Neural Network<br />

5.3 Results<br />

5.3.1 Simulated <strong>Data</strong><br />

In a Monte Carlo simulation, 20 000 alpha <strong>and</strong> beta events were generated all over the Inner<br />

Vessel, with r<strong>and</strong>om energies from 0 to 3 MeV. Fig. 5.6 shows a typical simulated alpha <strong>and</strong> a<br />

beta pulse for the CTF2 geometry. The time spectrum recorded was binned in such a way to<br />

reproduce the flash ADC output (2.5 ns sampling time, 8 bit depth).<br />

The input values for the NN were:<br />

- 100 bins <strong>of</strong> the normalized flash ADC spectrum (250 ns);<br />

- the radial distance from the center (reconstructed position), normalized to the Inner<br />

Vessel radius;<br />

- the energy <strong>of</strong> the event, in MeV.<br />

The NN had 102 neurons in the input layer, 102 neurons in the hidden layer, <strong>and</strong> 1 neuron in<br />

the output layer, giving ¢ weights Û. The output parameter <strong>of</strong> the<br />

net is called nn¬ <strong>and</strong> can take values between 0 <strong>and</strong> 1. Ideally it should be 1 for beta events<br />

<strong>and</strong> 0 for alpha events. If nn¬ is between 0 <strong>and</strong> 0.5, the event is classified as alpha event; if<br />

nn¬ is larger than 0.5, the event is classified as beta event. The training set consisted <strong>of</strong> 8000<br />

events. After each 10 events the weights were updated using the backpropagation algorithm.<br />

The validation set consisted <strong>of</strong> 8000 events (different from the training set). The results <strong>of</strong><br />

the NN after 5000 generations are shown in in fig. 5.7 for events with energies greater than<br />

0.2 MeV. From 3629 beta events only 46 were misidentified as alpha events. From 3607 alpha<br />

events 42 were misidentified as beta events. This means, that for 98.7 % beta identification<br />

efficiency, 98.8 % <strong>of</strong> the alpha events are rejected.<br />

For a comparison I also calculated the tail-total-ratio from the flash ADC spectrum with the<br />

tail starting after 47.5 ns (see fig. 5.8). For the same beta identification efficiency (98.7 %) with<br />

this method, I also got the same alpha rejection efficiency (98.8 %).<br />

The neural network has the same discrimination capability as the st<strong>and</strong>ard tail-to-total ratio,<br />

but it cannot beat this simpler <strong>and</strong> more straightforward technique.<br />

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