Step 1: Nature of species that show unimolecular behavior.
The Lindemann–Hinshelwood (L–H) scheme explains unimolecular reactions such as isomerizations and decompositions in the gas phase. Energy randomization within an \emph{activated} molecule requires multiple internal degrees of freedom; therefore it is typically valid for polyatomic (}\(\ge 3\)\textbf{-atom) molecules. Hence statement (A) is true.
Step 2: Elementary steps in the L–H mechanism.
The mechanism proceeds via:
\[
\mathrm{A + M \xrightleftharpoons[k_{-1}]{k_1} A^{*} + M} \quad \text{(bimolecular activation/deactivation)}
\]
\[
\mathrm{A^{*} \xrightarrow{k_2} \text{Products}} \quad \text{(unimolecular decomposition)}
\]
Thus, it \emph{does} involve bimolecular elementary steps (A + M), so (B) is true.
Step 3: Pressure dependence of the overall rate law.
At low pressure, activation collisions are infrequent, and the rate is proportional to \([A][M]\), i.e., second order. Hence (C) is true.
At high pressure, rapid activation makes decomposition of \(A^{*}\) rate-determining, giving a first-order overall rate. Therefore (D) is false.
\[
\boxed{\text{True statements: A, B, and C.}}
\]