  The hadronic charmless B decays into a scalar meson and a pseudoscalar meson
are studied within the framework of QCD factorization. Although the light
scalar mesons $f_0(980)$ and $a_0(980)$ are widely perceived as primarily the
four-quark bound states, in practice it is difficult to make quantitative
predictions based on the four-quark picture for light scalars. Hence,
predictions are made in the 2-quark model for the scalar mesons. Based on the
QCD sum rule method, we have derived the leading-twist light-cone distribution
amplitudes of scalar mesons and their decay constants. The short-distance
approach suffices to explain the observed large rates of $f_0(980)K^-$ and
$f_0(980)\bar K^0$ that receive major penguin contributions from the $b\to
ss\bar s$ process. When $f_0(980)$ is assigned as a four-quark bound state,
there exist extra diagrams contributing to $B\to f_0(980)K$. Therefore, a
priori the $f_0(980)K$ rate is not necessarily suppressed for a four-quark
state $f_0(980)$. The calculated $\bar B^0\to a_0^+(980)\pi^-$ and
$a_0^+(980)K^-$ rates exceed slightly the current experimental limits. If the
branching ratio of $\bar B^0\to a_0^+(1450)\pi^-$ is measured at the level of
$(4\sim 6)\times 10^{-6}$ while $a_0^+(980)\pi^-$ is found to be smaller, say,
of order $(1\sim 2)\times 10^{-6}$ or even smaller than this, it will be likely
to imply a 2-quark nature for $a_0(1450)$ and a four-quark assignment for
$a_0(980)$. The penguin-dominated modes $a_0(980)K$ and $a_0(1450)K$ receive
dominant weak annihilation contributions.
