  We delineate the flat limit of massless scalar scattering in
$\mathrm{AdS}_2$. We derive the 1 $\to$ 1 $\mathcal{S}$-matrix from the CFT
$2$-point function, which is proportional to the momentum-conserving delta
function. We prove a kinematical characteristic of the $2 \to 2$
$\mathcal{S}$-matrix in $2d$, elucidating the presence of product of two delta
functions arising from the $\phi^4$ contact interaction within the realm of the
flat limit of AdS/CFT. We also show that the factorization of the $n \to n
~\mathcal{S}$-matrix for integrable models in the flat limit, employing a
focused analysis on contact interaction, which play a pivotal role as
fundamental constituents in the construction of the non-perturbative
$\mathcal{S}$-matrix within integrable models. Although the factorization of
the $\mathcal{S}$-matrix in integrable models is commonly perceived as an
intrinsically non-perturbative notion, we effectively demonstrate its
manifestation at the tree level in the flat limit. We calculate the
$\mathcal{S}$-matrix by making use of the mapping between the CFT operator on
the AdS boundary, and the scattering state in flat space. We adopt the bulk
operator reconstruction to examine massless scalar scattering in the flat
limit. We solve the Klein-Gordon equation in the global $\mathrm{AdS}_2$ for
the massless scalar field. Notably, the solution is remarkably simple,
characterized by a pure phase in global time and a sinusoidal function in the
radial coordinate. This simplicity extends to the smearing function, enabling a
mapping between the scattering state and CFT operator taking AdS corrections
into account.
