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Remarkable stability of γ - N 2 and its prevalence in the nitrogen phase diagram.
Yan, Jinwei; Dalladay-Simpson, Philip; Conway, Lewis J; Gorelli, Federico; Pickard, Chris; Liu, Xiao-Di; Gregoryanz, Eugene.
Affiliation
  • Yan J; Key Laboratory of Materials Physics, Institute of Solid State Physics, HFIPS, Chinese Academy of Sciences, Hefei, 230031, China.
  • Dalladay-Simpson P; Center for High Pressure Science and Technology Advanced Research, Shanghai, China.
  • Conway LJ; Centre for Science at Extreme Conditions and School of Physics an Astronomy, University of Edinburgh, Edinburgh, UK.
  • Gorelli F; University of Science and Technology of China, Hefei, China.
  • Pickard C; Center for High Pressure Science and Technology Advanced Research, Shanghai, China. philip.dalladay-simpson@hpstar.ac.cn.
  • Liu XD; Department of Materials Science and Metallurgy, University of Cambridge, 27 Charles Babbage Road, Cambridge, CB30FS, UK.
  • Gregoryanz E; Advanced Institute for Materials Research, Tohoku University, Sendai, 980-8577, Japan.
Sci Rep ; 14(1): 16394, 2024 Jul 16.
Article in En | MEDLINE | ID: mdl-39014016
ABSTRACT
Solid nitrogen exhibits a panoply of phenomena ranging from complex molecular crystalline configurations to polymerization and closing band gap at higher densities. Among the elemental molecular solids, nitrogen stands apart for having phases, which can only be stabilized following particular pressure-temperature pathways, indicative of metastability and kinetic barriers. Here, through the combination of Raman spectroscopy and dynamic compression techniques, we find that the appearance of the whole nitrogen phase diagram is determined by the P-T paths taken below 2 GPa. We reveal the existence of the path- and phase-dependent triple point between the ß - N 2 , δ loc - N 2 and γ - or ϵ - N 2 . We further show that the ß - N 2 towards γ - N 2 path below the triple point, that evades δ ( δ loc )- N 2 , results in the formation of γ - N 2 , which in turn becomes a dominant phase. We then demonstrate, that the ß - N 2 through δ ( δ loc )- N 2 above the triple point path leads to the formation of ϵ - N 2 and the "well-established" phase diagram. An additional pathway, which by-passes the rotationally inhibited modifications δ ( δ loc )- N 2 , via rapid compression is found to produce γ - N 2 at higher temperatures. We argue that the pathway and phase sensitive triple point and the compression rate dependent phase formation challenge our understanding of this archetypal dense molecular solid.