Table 3: Fluence upper limits ($90\%$ C.L.) for neutrinos of different energies, obtained from IBD and NC classes of events.
$E_{\nu}$ $\delta t = 20$ s   $\delta t = 100$ s  
  $\Phi_{\bar\nu_{\rm e}}$ $\rm [cm^{-2}]$ $\Phi_{\nu_i}$ $\rm [cm^{-2}]$ $\Phi_{\bar\nu_{\rm e}}$ $\rm [cm^{-2}]$ $\Phi_{\nu_i}$ $\rm [cm^{-2}]$
10 MeV $4.64\times 10^{9}$ - $9.85\times10^{9}$ -
15 MeV $1.94\times 10^{9}$ - $4.13\times 10^{9}$ -
20 MeV $1.08\times 10^{9}$ $1.29\times 10^{11}$ $2.30\times 10^{9}$ $3.32\times 10^{11}$
30 MeV $4.97\times 10^{8}$ $1.51\times 10^{10}$ $1.05\times 10^{9}$ $3.90\times 10^{10}$
40 MeV $2.94\times 10^{8}$ $6.06\times 10^{9}$ $6.25\times 10^{8}$ $1.56\times 10^{10}$
50 MeV $2.00\times 10^{8}$ $3.54\times 10^{9}$ $4.25\times 10^{8}$ $9.10\times 10^{9}$
60 MeV $1.48\times 10^{8}$ $2.50\times 10^{9}$ $3.15\times 10^{8}$ $6.44\times 10^{9}$
70 MeV $1.16\times10^{8}$ $2.01\times 10^{9}$ $2.47\times 10^{8}$ $5.18\times 10^{9}$
80 MeV $9.52\times 10^{7}$ $1.74\times 10^{9}$ $2.02\times 10^{8}$ $4.48\times 10^{9}$
90 MeV $7.85\times 10^{7}$ $1.60\times 10^{9}$ $1.67\times 10^{8}$ $4.12\times 10^{9}$
100 MeV $6.89\times10^{7}$ $1.53\times 10^{9}$ $1.46\times 10^{8}$ $3.93\times 10^{9}$


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