“…Canonical double-stranded DNA structures are usually very stable under pressure. ,, Polymeric B-DNA structures with melting temperatures, T m , beyond about 50 °C are usually stabilized against unfolding upon pressurization, i.e ., the helix-to-coil transition of DNA is accompanied by a positive overall volume change, Δ V , suggesting that a positive thermal/hydration volume contribution outweighs a negative void volume contribution to Δ V at high temperatures, leading to positive values of the Clapeyron transition slope, d T m /d p . ,,, The stability of helical nucleic acid structures was found to be quite high because they are rather densely packed and their conformation is largely controlled by hydrogen bonds and π–π-stacking interactions between aromatic rings, which are not significantly affected or even stabilized by high pressure. This high stability of B-DNAs is generally not observed in the case of RNAs, ribozymes, and noncanonical DNA/RNA structures, where bends, twists, and cavities are structural features, similar to proteins, and consequently pressure-induced changes can alter their biochemical activities. ,,− The tRNA Phe showed small negative volume changes upon unfolding, the pressure-dependent structural changes being rather small, however, with a maximum of about 15% unpaired bases observed upon pressurization up to 10 kbar . Pioneered by Sugimoto, Chalikian, Macgregor, and their co-workers, it was found that noncanonical nucleic acid structure, including DNA hairpins (DNA-HPs), G-quadruplexes (G4Qs), and i-motifs, are pretty pressure-sensitive, and their pressure-sensitivity varies with their base sequence and the type and concentration of the counterions present in solution. − …”