$\Rightarrow \frac{ R _{1}}{ R _{2}}=\frac{\frac{ mv _{1}}{ q _{1} B }}{\frac{ mv _{2}}{ q _{2} B }}=\frac{ v _{1}}{ q _{1}} \times \frac{ q _{2}}{ v _{2}}=\frac{ q _{2}}{ q _{1}} \times \frac{ v _{1}}{ v _{2}}$
$=\frac{2}{ l } \times\left(\frac{2}{3}\right)=\frac{4}{3}$

$(A)$ If $I_1=I_2$, then B' cannot be equal to zero at the origin $(0,0,0)$
$(B)$ If $\mathrm{I}_1>0$ and $\mathrm{I}_2<0$, then $\mathrm{B}$ can be equal to zero at the origin $(0,0,0)$
$(C)$ If $\mathrm{I}_1<0$ and $\mathrm{I}_2>0$, then $\mathrm{B}$ can be equal to zero at the origin $(0,0,0)$
$(D)$ If $\mathrm{I}_1=\mathrm{I}_2$, then the $\mathrm{z}$-component of the magnetic field at the centre of the loop is $\left(-\frac{\mu_0 \mathrm{I}}{2 \mathrm{R}}\right)$
