Fig. 5.

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Comparison of the signal-selection efficiency for the RTS2 method (solid line) and for the multiplicity method (dashed line = time window of 20 s, dotted line = time window of 5 s), as a function of the number of true signal neutrinos in the detected burst, for FAR = 1 century−1, different background rates r = 0.01 − 0.1 s−1, and different values of the signal shape parameter τ2.
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