Structural and Electronic Competing Mechanisms in the Formation of Amorphous Carbon Nitride by Compressing s-Triazine

被引:30
作者
Citroni, Margherita [1 ,2 ]
Fanetti, Samuele [2 ]
Bazzicalupi, Carla [1 ]
Dziubek, Kamil [2 ,3 ]
Pagliai, Marco [1 ]
Nobrega, Marcelo Medre [4 ]
Mezouar, Mohamed [5 ]
Bini, Roberto [1 ,2 ]
机构
[1] Univ Florence, Dipartimento Chim Ugo Schiff, I-50019 Florence, Italy
[2] LENS, I-50019 Florence, Italy
[3] Adam Mickiewicz Univ, Fac Chem, PL-61614 Poznan, Poland
[4] Univ Sao Paulo, Inst Quim, Dept Quim Fundamental, BR-05513970 Sao Paulo, SP, Brazil
[5] European Synchrotron Radiat Facil, F-38043 Grenoble, France
基金
巴西圣保罗研究基金会;
关键词
SOLID-STATE NMR; HIGH-PRESSURE; PHASE-TRANSITION; CRYSTAL-STRUCTURE; FORM; C6N9H3-CENTER-DOT-HCL; SPECTROSCOPY; DIFFRACTION; SCATTERING; DYNAMICS;
D O I
10.1021/acs.jpcc.5b09538
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
The pressure-induced transformation of molecular crystals can give rise to new materials characterized by intriguing hardness Or energetic properties. Mechanisms regulating these reactions at the molecular level result from a complex interplay among crystal structure, lattice dynamics, and electronic properties. Here, we show that the formation of a three-dimensional amorphous carbon nitride by compressing phase II s-triazine is controlled by the competition between two different mechanisms, one entirely structural and the other electronic, representing the first example where such occurrence is demonstrated. Temperature drives the reactivity below 8 GP a by ruling the lattice dynamics, whereas above 8 GPa the electronic modifications, uniquely governed by pressure, trigger the chemical transformation. The amorphous material synthesized has a bonding structure characterized by a bulk typical of a strongly conjugated three-dimensional carbon nitride with hydrogen atoms Migrated to saturate C and N terminations.
引用
收藏
页码:28560 / 28569
页数:10
相关论文
共 62 条
[1]  
Agrawal J.P., 2010, High Energy Materials
[2]   On a new model of the graphitic form of C3N4 [J].
Alves, I ;
Demazeau, G ;
Tanguy, B ;
Weill, F .
SOLID STATE COMMUNICATIONS, 1999, 109 (11) :697-701
[3]  
[Anonymous], 2009, TOPAS VERS 4 2
[4]   Granulation, Phase Change, and Microstructure - Kinetics of Phase Change. III [J].
Avrami, M .
JOURNAL OF CHEMICAL PHYSICS, 1941, 9 (02) :177-184
[5]   Kinetics of phase change I - General theory [J].
Avrami, M .
JOURNAL OF CHEMICAL PHYSICS, 1939, 7 (12) :1103-1112
[6]  
Avrami M., 1940, J CHEM PHYS, V8, P212, DOI [10.1063/1.1750631, DOI 10.1063/1.1750631]
[7]   DENSITY-FUNCTIONAL EXCHANGE-ENERGY APPROXIMATION WITH CORRECT ASYMPTOTIC-BEHAVIOR [J].
BECKE, AD .
PHYSICAL REVIEW A, 1988, 38 (06) :3098-3100
[8]   Experimental setup for Fourier transform infrared spectroscopy studies in condensed matter at high pressure and low temperatures [J].
Bini, R ;
Ballerini, R ;
Pratesi, G ;
Jodl, HJ .
REVIEW OF SCIENTIFIC INSTRUMENTS, 1997, 68 (08) :3154-3160
[9]  
Bini R., 2014, Materials under extreme conditions: molecular crystals at high pressure
[10]   UNIFIED APPROACH FOR MOLECULAR-DYNAMICS AND DENSITY-FUNCTIONAL THEORY [J].
CAR, R ;
PARRINELLO, M .
PHYSICAL REVIEW LETTERS, 1985, 55 (22) :2471-2474