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 redistribution inside an activated molecule requires many internal degrees of freedom. This is generally possible only in polyatomic molecules (≥ 3 atoms). Hence, statement (A) is true.
Step 2: Elementary steps in the L–H mechanism.
The mechanism involves two stages:
\[
\mathrm{A + M \xrightleftharpoons[k_{-1}]{k_1} A^{*} + M} \quad \text{(bimolecular activation/deactivation)}
\]
\[
\mathrm{A^{*} \xrightarrow{k_2} \text{Products}} \quad \text{(unimolecular decomposition)}
\]
Thus, the scheme does include bimolecular steps (A + M collisions), making statement (B) true.
Step 3: Pressure dependence of the overall rate law.
At low pressure, collisions between A and M are rare, so the formation of A* is slow. The rate is proportional to \([A][M]\), giving an overall second-order rate law. Hence, statement (C) is true.
At high pressure, activation to A* is rapid and essentially in equilibrium. The slow step is the unimolecular decomposition of A*, so the overall reaction becomes first order in [A]. Therefore, statement (D) is false.
Final Answer: The correct true statements are A, B, and C.