  In this paper, we investigate the boundedness of bilinear Calder\'on-Zygmund
operators $T$ from ${L^{p_1}\left(w_1\right)} \times {L^{p_2}\left(w_2\right)}$
to ${L^{p,\infty}\left(v_{\vec{w}}\right)}$ with the stopping time method,
where $1 / p = 1 / p_1 + 1 / p_2$ , $1 < p_1, p_2 < \infty$ and $\vec{w}$ is a
multiple $A_{\vec{P}}$ weight. Specifically, we studied the exponent $\alpha$
of $A_{\vec{P}}$ constant in formula
$$\|T(\vec{f})\|_{L^{p,\infty}\left(v_{\vec{w}}\right)} \leqslant C_{m, n,
\vec{P},
T}[\vec{w}]_{A_{\vec{P}}}^{\alpha}\left\|f_1\right\|_{L^{p_1}\left(w_1\right)}\left\|f_2\right\|_{L^{p_2}\left(w_2\right)}.$$
Surprisingly, we show that when $p \geqslant \frac{3+\sqrt{5}}{2}$ or
$\min\{p_1,p_2\} > 4$, the index $\alpha$ in the above equation can be less
than $1$, which is different from the linear scenario.
