Step 1: The parent particle is at rest, so total momentum is zero. By conservation of momentum the two daughters must carry equal and opposite momenta, hence equal speeds in opposite directions along the z-axis: \(\vec{v}_1 = -\vec{v}_2\).
Step 2: Conserve total (relativistic) energy. The initial energy is the rest energy \(mc^2\). Each daughter has energy \(\gamma\left(\tfrac{3}{10}m\right)c^2\), so \[2\,\gamma\left(\tfrac{3}{10}m\right)c^2 = mc^2.\]
Step 3: Solve for the Lorentz factor: \[\gamma = \frac{mc^2}{2\cdot\tfrac{3}{10}mc^2} = \frac{10}{6} = \frac{5}{3}.\]
Step 4: Recover the speed from \(\gamma = \dfrac{1}{\sqrt{1-v^2/c^2}}\): \[1-\frac{v^2}{c^2} = \frac{1}{\gamma^2} = \frac{9}{25} \;\Rightarrow\; \frac{v^2}{c^2} = \frac{16}{25} \;\Rightarrow\; v = 0.8c.\]
Step 5: The daughters move oppositely along z, so \(v_1 = -v_2 = 0.8c\,\hat{z}\).\[\boxed{v_1 = -v_2 = 0.8c\,\hat{z}}\]