Chem. J. Chinese Universities ›› 2005, Vol. 26 ›› Issue (5): 811.

• Articles • Previous Articles     Next Articles

Preparation and Characterization of BCN

BAI Suo-Zhu1,4, YAO Bin1,3, HUANG Bao-Kun1, ZHANG Shi-Jing1, DING Zhan-Hui1, GUO Xing-Yuan1, ZHOU Xiang-Dong1, SU Wen-Hui1,2,3   

  1. 1. College of Physics, Jilin University, Changchun 130023, China;
    2. Center for Condensed Matter Science and Technology, Harbin Institute of Technology, Harbin 150001, China;
    3. International Center for Materials Physics, Chinese Academy of Sciences, Shenyang 110015, China;
    4. Chemistry College, Inner Mongolia University for Nationalities, Tongliao 028043, China
  • Received:2004-07-06 Online:2005-05-10 Published:2005-05-10

Abstract: Formation, structure and phase transition of BCN compound were investigated by mechanical milling of mixture of graphite and hexagonal boron nitride or annealing the as-milled mixture at high temperature and high pressure. Amorphous BCN(a-BCN) was prepared by milling the mixture for 120 h. A broad and strong absorbed peak locating at 1 400 cm-1 and two weak peaks locating at 740 and 1 630 cm-1 respectively were observed in the infrared spectrum of the a-BCN, and a broad (Raman) scattering peak was found at 1 330 cm-1 in its Raman spectrum. The binding energies of the (a-BCN) are 191.9 eV for B1s, 284.9 and 286.8 eV for C1s, 398.3 and 400.5 eV for N1s, respectively. (A hexagonal) BCN(h-BCN) with lattice constants of a=0.250 5 nm, c=0. 666 4 nm was produced by annealing the a-BCN for 45 min at 1 473 K and 4 GPa. Its infrared absorbed peaks appeared at 1 398, 1 103, 1 024, 925 and 802 cm-1, respectively, and Raman scattering peaks are observed at 1 328, (1 358), 1 582 and 1 614 cm-1, respectively. The mechanisms of the formation and phase transition of the BCN compound are discussed.

Key words: B—C—N, Mechanical milling, High temperature and high pressure, Raman spectrum, (Infrared) spectrum

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