  The decays of $B_{d,s}^0 \to \sigma\sigma, \sigma f_0, f_0 f_0$, with
$\sigma$ and $f_0$ denoting the light scalar mesons $f_0(500)$ and $f_0(980)$
in the two-quark picture, are studied in the perturbative QCD approach based on
$k_T$ factorization. With the referenced value of the mixing angle $|\varphi|
\sim 25^\circ$ for the $\sigma-f_0$ mixing in the quark-flavor basis, it is of
great interest to obtain that: (a) these neutral $B$-meson decays into
$\sigma\sigma, \sigma f_0$, and $f_0 f_0$ have large branching ratios in the
order of $10^{-6} \sim 10^{-4}$, which mean the possibly constructive
interferences existed in the decays with different flavor states, and then are
expected to be tested at the Large Hadron Collider beauty and/or Belle-II
experiments in the (near) future; (b) the large direct CP violations could be
easily found in the $B_d^0 \to \sigma\sigma, f_0 f_0$ and $B_{d,s}^0 \to \sigma
f_0$ decays, which indicate the considerable interferences between the tree and
the penguin decay amplitudes involved in these four modes, and would be
confronted with the future measurements; (c) these neutral $B$-meson decays
could be examined through the secondary decay chain $\sigma/f_0 \to \pi^+
\pi^-$, namely, the four-body decays of $B_{d,s}^0 \to (\pi^+
\pi^-)_{\sigma(f_0)} (\pi^+ \pi^-)_{\sigma(f_0)}$. On the other side, it seems
that other 4 four-body decays of $B_d^0 \to (\pi^+ \pi^-)_{\sigma} (K^+
K^-)_{f_0}$, $B_s^0 \to (\pi^+ \pi^-)_{\sigma(f_0)} (K^+ K^-)_{f_0}$, and
$B_s^0 \to (K^+ K^-)_{f_0} (K^+ K^-)_{f_0}$ could also be detected at the
relevant experiments, if the $f_0 \to K^+ K^-$ could be identified from the
$\phi \to K^+ K^-$ clearly.
