Electroconductivity and pressure-temperature states of step shocked C60 fullerite

被引:2
作者
Molodets, A. M. [1 ]
Avdonin, V. V.
Zhukov, A. N.
Kim, V. V.
Osip'yan, A. Yu.
Sidorov, N. S.
Shulga, J. M.
Fortov, V. E.
机构
[1] Russian Acad Sci, Inst Problems Chem Phys, Chernogolovka 142432, Russia
[2] Russian Acad Sci, Inst Solid State Phys, Chernogolovka 142432, Russia
关键词
high pressure; equation of state; conductivity; fullerenes; hugoniot;
D O I
10.1080/08957950701211072
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
A study of electrophysical and thermodynamic properties of C-60 single crystals under step shock loading has been carried out. The increase and the following reduction in specific electroconductivity of C-60 fullerite single crystals at step shock compression up to pressure 30 GPa have been measured. The equations of state for face centred cubic (fcc) C-60 fullerite as well as for two-dimensional polymer C-60 and for three-dimensional polymer C-60 (3D-C-60) were constructed. The pressure-temperature states of C-60 fullerite were calculated at step shock compression up to pressure 30 GPa and temperature 550 K. The X-ray diffraction studies of shock-recovered samples reveal a mixture of fcc C-60 and a X-ray amorphous component of fullerite C-60. The start of the formation of the X-ray amorphous component occurs at a pressure P-m approximate to 19.8 GPa and a temperature T-m approximate to 520 K. At pressures exceeding P-m and temperatures exceeding T-m, the shock compressed fullerite consist of a two-phase mixture of fcc C-60 fullerite and an X-ray amorphous component presumably consisting of the nucleators of polymer 3D-C-60 fullerite. The decrease in electroconductivity of fullerite can be explained by the percolation effect caused by the change of pressure, size and number of polymeric phase nuclei.
引用
收藏
页码:279 / 290
页数:12
相关论文
共 21 条
[1]   Interplay between the structure and properties of new metastable carbon phases obtained under high pressures from fullerite C60 and carbyne [J].
Brazhkin, VV ;
Lyapin, AG ;
Popova, SV ;
Bayliss, SC ;
Varfolomeeva, TD ;
Voloshin, RN ;
Gavrilyuk, AG ;
Kondrin, MV ;
Mukhamad'yarov, VV ;
Troyan, IA ;
Demishev, SV ;
Pronin, AA ;
Sluchanko, NE .
JETP LETTERS, 2002, 76 (11) :681-692
[2]  
Bushman A. V., 1988, THERMAL PHYS DYNAMIC
[3]  
BUSHMAN AA, 1989, MODELS WIDE RANGE EQ
[4]  
DAVYDOV VA, 2001, J RUS CHEM SOC, V45, P25
[5]  
Diky V.V., 2000, Russian Chemical Reviews, V69, P95, DOI [10.1070/RC2000v069n02ABEH000535, DOI 10.1070/RC2000V069N02ABEH000535]
[6]   GRAPHITE UNDER PRESSURE - EQUATION OF STATE AND 1ST-ORDER RAMAN MODES [J].
HANFLAND, M ;
BEISTER, H ;
SYASSEN, K .
PHYSICAL REVIEW B, 1989, 39 (17) :12598-12603
[7]   Compressibility measurement of C60 using synchrotron radiation [J].
Horikawa, T ;
Kinoshita, T ;
Suito, K ;
Onodera, A .
SOLID STATE COMMUNICATIONS, 2000, 114 (03) :121-125
[8]   THERMODYNAMIC CHARACTERIZATION OF C-60 BY DIFFERENTIAL SCANNING CALORIMETRY [J].
JIN, YM ;
CHENG, JL ;
VARMANAIR, M ;
LIANG, GH ;
FU, YG ;
WUNDERLICH, B ;
XIANG, XD ;
MOSTOVOY, R ;
ZETTL, AK .
JOURNAL OF PHYSICAL CHEMISTRY, 1992, 96 (12) :5151-5156
[9]  
KANEL GI, 1974, FIZ GORENIA I VZRIVA, V6, P884
[10]  
KIM VV, 2005, COMPUTATIONAL MODELI