= \^3,   \_2 = - ,   \_2 = , \[eq;tilde\_values\_d-wave\]\
&& \_3 = \^5,   \_3 = - \^3,   \_3 = ,     \_3 = - . \[eq;tilde\_values\_f-wave\] Those values (and variations from them for some terms) are used as the initial input of the effective range parameters for the parameter fitting.[^5]

[c|cccc|cc]{} & $a_0$ (fm) & $r_0$ (fm) & $P_0$ (fm$^3$) & $Q_0$ (fm$^5$) & $ReD_{0G}$ (MeV) & $|C_b|$ (fm$^{-1/2}$) $S0$ & $6.2\times 10^4$ & 0.268514(3) & $-0.0343(4)$ & 0.0019(2) & $4.2(7)\times 10^{-3}$ & $6.8(16)\times 10^2$ $S1$ & $6.6\times 10^4$ & 0.268514(3) & $-0.0342(3)$ & 0.0020(3) & $4.0(5)\times 10^{-3}$ & $7.4(15)\times 10^2$ $S2$ & $5.8\times 10^4$ & 0.268513(3) & $-0.0345(2)$ & 0.0018(1) & $4.4(4)\times 10^{-3}$ & $6.4(7)\times 10^2$ & — & $\tilde{r}_0$ (fm) & $\tilde{P}_0$ (fm$^3$) & $\tilde{Q}_0$ (fm$^5$) & — & — & — & 0.268735 & $-0.0349$ & 0.0027 & — & —

[c|cccc|cc]{} &$a_1$(fm$^3$)& $r_1$ (fm$^{-1}$) & $P_1$ (fm) & $Q_1$ (fm$^3$) & $ReD_{1G}$ (MeV$^3$) & $|C_b|$ (fm$^{-1/2}$) $P0$ & $-1.8\times 10^5$ & 0.4150(6) & $-0.577(8)$ & 0.019(3) & $2.7(8)\times 10^2$ & $1.9(4)\times 10^{14}$ $P1$ & $-1.6\times 10^5$ & 0.4153(2) & $-0.574(2)$ & 0.020(1) & $3.0(3)\times 10^2$ & $1.8(1)\times 10^{14}$ $P2$ & $-1.3\times 10^5$ & 0.4157(2) & $-0.569(2)$ 