There is an incentive for research directed towards new environmentally friendly oxidizers and energetic materials. [1][2][3] Recent examples for advances in polynitrogen chemistry are the bulk synthesis of the V-shaped N 5 + , [4,5] the tetrazole-based CN 7 , À[6] and the detection of cyclic N 5 À . [7,8] Compounds containing exclusively oxygen and nitrogen are desirable for applications such as environmentally benign rocket propulsion. Of those, the dinitramide anion (N-(NO 2 ) 2 À ) [9][10][11] is the heaviest compound known to date. Trinitramide (TNA; N(NO 2 ) 3 ) constitutes a possible energetic green oxidizer that could be suitable for future high-performance propellants. Only a few theoretical works have previously dealt with this hitherto unknown nitrogen oxide. [12][13][14] The heat of formation (DH 0 f(gas) ) of TNA has been estimated at between 38 and 71 kcal mol À1 , [12][13][14] and the N À N bond dissociation energy has been estimated to be 20-27 kcal mol À1 . [13,14] The existence of an N 4 O 6 intermediate has also been speculated to explain observed decomposition kinetics of dinitraminic acid (HN(NO 2 ) 2 ) in nitric acid.[15] To the best of our knowledge, no synthetic effort toward TNA has been attempted. Herein we present the first experimental detection of this exotic molecule.We initially subjected TNA to a thorough quantum chemical analysis. The aim of this study was to decipher the kinetic stability and different decomposition pathways in gas phase and in solution. We also performed calculations on two possible synthesis routes, and estimated physical properties such as density, heat of formation, vaporization, sublimation, and performance characteristics of TNA as a rocket-propellant component.Proposed self-decomposition pathways available to TNA are shown in Scheme 1. The NÀN bond dissociation enthalpy in the gas phase is calculated to be 28.2 kcal mol À1 . Owing to the favorable change in entropy, this dissociation is likely the dominant route for decomposition in the gas phase. The transition state TS1 (Scheme 1) was found to be in close competition with the homolytic bond fission, with a barrier corresponding to a relative free energy of 27.9 kcal mol À1 . Surprisingly, DFT methods, such as the widely used B3LYP, or the more recent B2PLYP functional, fail in describing the energy landscape of both these pathways. The barrier heights are underestimated by 8-11 kcal mol À1 compared to CBS-QB3 (extrapolated CCSD(T)) and SCS-MP2 calculations, which are in very good agreement. As we know from previous studies that B3LYP, B2PLYP, and highlevel ab initio methods (such as CCSD(T) and SCS-MP2) behave very similarly when treating N(NO 2 ) 2 À and its radical, [16] and, given the high accuracy of the latter methods, we can safely assume that the error by DFT stems from an overestimation of the TNA ground state energy. Thus, the limited interest in TNA might be caused by the wide use of B3LYP, which underestimates its stability.The character of TS1 is between a NO 2 radical and a NO 2 cation tran...