TY - JOUR
T1 - High-energy-density polymeric carbon oxide
T2 - Layered Cx Oy solids under pressure
AU - Sun, Chuli
AU - Guo, Wei
AU - Zhu, Jinlong
AU - Li, Xiang
AU - Yao, Yugui
N1 - Publisher Copyright:
© 2021 American Physical Society.
PY - 2021/9/1
Y1 - 2021/9/1
N2 - Pressure-induced polymerization of carbon monoxide (CO) molecules may lead to next-generation high energy density materials. By combining structural search method, first-principles calculations and ab initio molecular dynamics (AIMD) simulations, we predict several polymeric carbon oxide CxOy, i.e., C5O2 (P-4m2), C6O4 (P-4m2 and I-4m2) and C8O8 (I-4m2), which are all layered semiconductors with high energy density, large bulk modulus, and high hardness. For the C:Oratio=1:1, the C8O8-I-4m2 phase is energetically more stable than the reported Cmca and Cmcm phases above 90 GPa, and its energy density is 4.51 kJ/g, which is higher than trinitrotoluene (TNT). Considering the mechanism of CO2 release, CxOy(x>y) crystals, namely C5O2 (P-4m2) and C6O4 (P-4m2 and I-4m2) are predicted above 40∼50GPa. At 100 GPa, phonon spectrum calculations and AIMD simulations indicate that they have good mechanical and dynamic stability. At 0 GPa, AIMD simulations also show the possible phase transition path of the four CxOy structures by releasing CO2: C8O8-I-4m2→C6O4-I-4m2 and C6O4-P-4m2→C5O2-P-4m2, and C6O4-I-4m2 and C5O2-P-4m2 can remain stable at ambient conditions. Those structures may enrich the phase diagram of high-pressure CxOy, and provide clues for synthesis and exploration of new stable energetic materials besides polymeric nitrogen.
AB - Pressure-induced polymerization of carbon monoxide (CO) molecules may lead to next-generation high energy density materials. By combining structural search method, first-principles calculations and ab initio molecular dynamics (AIMD) simulations, we predict several polymeric carbon oxide CxOy, i.e., C5O2 (P-4m2), C6O4 (P-4m2 and I-4m2) and C8O8 (I-4m2), which are all layered semiconductors with high energy density, large bulk modulus, and high hardness. For the C:Oratio=1:1, the C8O8-I-4m2 phase is energetically more stable than the reported Cmca and Cmcm phases above 90 GPa, and its energy density is 4.51 kJ/g, which is higher than trinitrotoluene (TNT). Considering the mechanism of CO2 release, CxOy(x>y) crystals, namely C5O2 (P-4m2) and C6O4 (P-4m2 and I-4m2) are predicted above 40∼50GPa. At 100 GPa, phonon spectrum calculations and AIMD simulations indicate that they have good mechanical and dynamic stability. At 0 GPa, AIMD simulations also show the possible phase transition path of the four CxOy structures by releasing CO2: C8O8-I-4m2→C6O4-I-4m2 and C6O4-P-4m2→C5O2-P-4m2, and C6O4-I-4m2 and C5O2-P-4m2 can remain stable at ambient conditions. Those structures may enrich the phase diagram of high-pressure CxOy, and provide clues for synthesis and exploration of new stable energetic materials besides polymeric nitrogen.
UR - http://www.scopus.com/inward/record.url?scp=85114892737&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.104.094102
DO - 10.1103/PhysRevB.104.094102
M3 - Article
AN - SCOPUS:85114892737
SN - 2469-9950
VL - 104
JO - Physical Review B
JF - Physical Review B
IS - 9
M1 - 094102
ER -