Structural polymorphism in dense carbon dioxide (CO 2 ) has attracted significant attention in high-pressure physics and chemistry for the past two decades. Here, we have performed high-pressure experiments and first-principles theoretical calculations to investigate the stability, structure, and dynamical properties of dense CO 2 . We found evidence that CO 2 -V with the 4-coordinated extended structure can be quenched to ambient pressure below 200 K-the melting temperature of CO 2 -I. CO 2 -V is a fully coordinated structure formed from a molecular solid at high pressure and recovered at ambient pressure. Apart from confirming the metastability of CO 2 -V (I-42d) at ambient pressure at low temperature, results of ab initio molecular dynamics and metadynamics (MD) simulations provided insights into the transformation processes and structural relationship from the molecular to the extended phases. In addition, the simulation also predicted a phase V′(Pna2 1 ) in the stability region of CO 2 -V with a diffraction pattern similar to that previously assigned to the CO 2 -V (P2 1 2 1 2 1 ) structure. Both CO 2 -V and -V′ are predicted to be recoverable and hard with a Vicker hardness of ∼20 GPa. Significantly, MD simulations found that the CO 2 in phase IV exhibits large-amplitude bending motions at finite temperatures and high pressures. This finding helps to explain the discrepancy between earlier predicted static structures and experiments. MD simulations clearly indicate temperature effects are critical to understanding the high-pressure behaviors of dense CO 2 structures-highlighting the significance of chemical kinetics associated with the transformations.carbon dioxide | molecular dynamics | high pressure | material science S olid carbon dioxide (CO 2 ) has a phase diagram rich in polymorphs, which exhibit great diversity in intermolecular interactions, chemical bonding, and crystal structures (1-7). Colloquially known as dry ice, solid CO 2 has a cubic Pa3 structure (phase I) under ambient pressure (8). At around 10 GPa, the cubic structure transforms to another molecular phase (Cmca, phase III) with different stacking pattern of CO 2 molecules. At sufficient compression, the molecular O = C = O bonds in solid CO 2 are replaced by an extended network of single C-O bonds, forming CO 4 tetrahedral units with sp 3 hybridized carbon atoms. The onset of such transformation occurs at 20 GPa, where the phase III transforms to a pseudotetragonal phase II (P4 2 /mnm or Pnnm) above ∼500 K and then to phase IV (P4 1 2 1 2 β-cristobalite structure) above ∼750 K (9-12). Continuing the compression to 40 GPa and then heating the product to 1,800 K, CO 2 further transforms to a nonmolecular polymeric strucutre V TD with the tridymite-like P2 1 2 1 2 1 structure (13, 14). Interestingly, following a different synthesis path, that is, heating the phase III first at 20 GPa and then compressing the product to 39 GPa and heating it again to ∼1,800 K, a different polymeric phase (CO 2 -V CR ) in a β-cristobalite-like I-42d structu...