— & —

In Tables \[table:s-wave\_parameters\], \[table:p-wave\_parameters\], \[table:d-wave\_parameters\], \[table:f-wave\_parameters\], fitted values and errors of the effective range parameters, $r_l$, $P_l$, $Q_l$, $R_l$ for $l=0,1,2,3$ channels to the data sets $\{S0, S1, S2\}$, $\{P0, P1, P2\}$, $\{D0, D1, D2\}$, $\{F0, F1, F2\}$, respectively, are presented. The errors of the fitted parameters stem from those of the phase shift data. Numerical values of the $\tilde{r}_l$, $\tilde{P}_l$, $\tilde{Q}_l$, $\tilde{R}_l$ terms for $l=0,1,2,3$ are also shown in the tables. The values of $a_l$ are calculated by using the fitted effective range parameters in Eq. (\[eq;moneoveral\]). The values in the second last column are the real part of the denominator $ReD_l(k)$ of the scattering amplitude at the energy corresponding to $T_G$ [^6] (i.e., at $k=k_G$), and those in the last column are the ANC, $|C_b|$, for the $0_2^+$, $1_1^-$, $2_1^+$, $3_1^-$ states.

One can see the errors of the fitted values of the effective range parameters are small, but the fitted effective range parameters are largely canceled with the corresponding $\tilde{r}_l$, $\tilde{P}_l$, $\tilde{Q}_l$, $\tilde{R}_l$ terms. In the values of the real part of denominator, $ReD_{lG}$, of the scattering amplitude at $k=k_G$, we find significant errors: about 9-17%, 9-30%, 16-94%, 9-10% errors, depending on the choice 