Table 1.

Values of the single candidate sensitivity ${\mathit{\alpha }}_{ij}$ and the number of candidates $N_{ij}^K$ compatible with the $K_{\mathrm{S}}^0$ mass (reconstructed mass in the range $[492,504]\mathrm{MeV}/c^2$), for each ${\text{BDT}}_{\mathrm{cb}}$ bin i and trigger category j. Only statistical uncertainties are given. The first uncertainty is uncorrelated, while the second is fully correlated among the ${\text{BDT}}_{\mathrm{cb}}$ bins of the same trigger category

Bin i	${\mathit{\alpha }}_{i{\text{TOS}}_{\mathit{\mu }}}(\times {10}^{-10})$	${\mathit{\alpha }}_{i{\text{TOS}}_{\mathit{\mu }\mathit{\mu }}}(\times {10}^{-9})$	$N_{i{\text{TOS}}_{\mathit{\mu }}}^K$	$N_{i{\text{TOS}}_{\mathit{\mu }\mathit{\mu }}}^K$
1	$7.48\pm 0.84\pm 0.16$	$5.30\pm 0.72\pm 0.12$	49	13
2	$7.72\pm 0.87\pm 0.17$	$4.71\pm 0.63\pm 0.10$	28	9
3	$7.85\pm 0.89\pm 0.18$	$4.88\pm 0.65\pm 0.11$	9	14
4	$7.93\pm 0.89\pm 0.19$	$4.66\pm 0.62\pm 0.10$	18	10
5	$7.53\pm 0.85\pm 0.18$	$4.65\pm 0.61\pm 0.10$	6	3
6	$7.78\pm 0.88\pm 0.19$	$4.95\pm 0.66\pm 0.11$	2	2
7	$7.56\pm 0.85\pm 0.19$	$4.60\pm 0.61\pm 0.10$	3	1
8	$7.90\pm 0.89\pm 0.19$	$5.00\pm 0.67\pm 0.11$	2	1
9	$7.81\pm 0.88\pm 0.18$	$4.72\pm 0.63\pm 0.11$	1	1
10	$7.75\pm 0.87\pm 0.17$	$4.66\pm 0.62\pm 0.11$	0	0