• The more stable syn-syn conformer of MA than the syn-anti conformer. • The preferred one-step process of Curtius rearrangement of syn-syn -MA comparing with the two-step concerted mechanism. • Eight structural stability domains and seven catastrophes of the cusp and fold types to achieve Curtius rearrangement of syn-syn -MA. • Ninet structural stability domains and eight catastrophes of the cusp and fold types to achieve Curtius rearrangement of syn-ICA. • The concerted Curtius rearrangement of syn-syn -MA and syn -ICA are highly asynchronous processes with the absolute asynchronicity of 0.801 and 0.763, respectively. An innovative and comprehensive theoretical investigation was conducted to examine the thermal Curtius rearrangement of malonyl azide in its syn–syn and syn–anti conformations, taking into account both the concerted and stepwise pathways. This study covered analyses performed in gaseous environments and a range of solvents. In both the gas phase and different solvents, the syn–syn conformation of malonyl azide proves to be more stable than the syn–anti conformation with a stability difference ranging from 4.15 to 4.99 kcal mol−1. It undergoes an exergonic concerted process with a single transition state, leading to the formation of syn –2–isocyanatoacetyl azide. Furthermore, syn –2–isocyanatoacetyl azide can be converted into methylene diisocyanate via a concerted pathway. In contrast, the rearrangement of the syn–anti conformation involves two transition states and an intermediate. The initial step is endergonic, followed by an exergonic subsequent step. The calculated ΔG values for the conversion of syn–syn –MA to syn –ICA and syn –ICA to MDI in the gas phase, determined at the CBS–QB3 level of theory, are –62.91 and –64.67 kcal mol−1, respectively. Meanwhile, the Gibbs free energies for the first and second steps of the rearrangement of syn-anti conformation are 10.51 and –77.98 kcal mol−1, respectively. Theoretical results indicate the dominance of the concerted pathway, surpassing the stepwise mechanism by roughly 104–106 and 104 times in both the gas phase and various solvents, respectively. Analyzing the electron localization function using the B3LYP/6–311++G(2d,d,p) level of theory unveils the catastrophe sequences for syn–syn malonyl azide and syn –2–isocyanatoacetyl azide structures, denoted as 8–CF†C†TSF†C†C†C and 9–CF†C†TSFC†FC†C-0 , respectively. The Curtius rearrangement of the syn–syn malonyl azide conformer commences with the transformation of two valence bonding disynaptic attractors, where V 1,2 (N 2 ,N 3) merges into a single disynaptic attractor. This is followed by the division of the non–bonding monosynaptic attractor V(N 1) into two non–bonding monosynaptic attractors. Subsequently, the N 1 –N 2 bond breaks, eliminating a nitrogen molecule and altering the topological signature of C 1 –N 1. This transformation leads to the consolidation of the pair of non–bonding monosynaptic attractors V 1,2 (N 1) into a single non–bonding monosynaptic attractor V(N 1). Then, the C 1 –C 2 bond breaks, resulting in the formation of pseudo–radical centers on the C 1 and C 2 atoms. Following this, a transformation in the topological signature of C 1 –N 1 occurs, leading to the elimination of pseudo–radical centers on the C 1 atom and the formation of a C 2 –N 1 bond. The results of ELF calculations indicate that the Curtius rearrangement of syn -ICA follows a method similar to that of syn-syn. The results indicate that the reaction follows a concerted mechanism but is highly asynchronous, with absolute asynchronicity indices of 0.801 and 0.763 for the Curtius rearrangement of syn -syn-MA and syn -ICA, respectively. [ABSTRACT FROM AUTHOR]