Pressure-induced amorphization and an amorphous-amorphous transition in densified porous silicon

被引:360
作者
Deb, SK
Wilding, M
Somayazulu, M
McMillan, PF
机构
[1] UCL, Christopher Ingold Labs, Dept Chem, London WC1H 0AJ, England
[2] Royal Inst Great Britain, Davy Faraday Res Lab, London W1X 4BS, England
[3] Argonne Natl Lab, Adv Photon Source, HPCAT, Argonne, IL 60439 USA
[4] Univ Calif Davis, Thermochem Facil, Davis, CA 95616 USA
[5] Bhabha Atom Res Ctr, Div Solid State Phys, Mumbai 400085, India
关键词
D O I
10.1038/35107036
中图分类号
O [数理科学和化学]; P [天文学、地球科学]; Q [生物科学]; N [自然科学总论];
学科分类号
07 ; 0710 ; 09 ;
摘要
Crystalline and amorphous forms of silicon are the principal materials used for solid-state electronics and photovoltaics technologies. Silicon is therefore a well-studied material, although new structures and properties are still being discovered(1-4). Compression of bulk silicon, which is tetrahedrally coordinated at atmospheric pressure, results in a transition to octahedrally coordinated metallic phases(5). In compressed nanocrystalline Si particles, the initial diamond structure persists to higher pressure than for bulk material, before transforming to high-density crystals(6). Here we report compression experiments on films of porous Si, which contains nanometre-sized domains of diamond-structured material(7-9). At pressures larger than 10 GPa we observed pressure-induced amorphization(10,11). Furthermore, we rnd from Raman spectroscopy measurements that the high-density amorphous form obtained by this process transforms to low-density amorphous silicon upon decompression. This amorphous-amorphous transition is remarkably similar to that reported previously for water(12,13), which suggests an underlying transition between a high-density and a low-density liquid phase in supercooled Si (refs 10, 14, 15). The Si melting temperature decreases with increasing pressure, and the crystalline semiconductor melts to a metallic liquid with average coordination similar to5 (ref. 16).
引用
收藏
页码:528 / 530
页数:3
相关论文
共 31 条
  • [1] ON TEMPERATURE DEPENDENCE OF COOPERATIVE RELAXATION PROPERTIES IN GLASS-FORMING LIQUIDS
    ADAM, G
    GIBBS, JH
    [J]. JOURNAL OF CHEMICAL PHYSICS, 1965, 43 (01) : 139 - &
  • [2] Angell CA, 1996, J NON-CRYST SOLIDS, V207, P463, DOI 10.1016/S0022-3093(96)00261-X
  • [3] 'Strong' and 'superstrong' liquids, and an approach to the perfect glass state via phase transition
    Angell, CA
    Moynihan, CT
    Hemmati, M
    [J]. JOURNAL OF NON-CRYSTALLINE SOLIDS, 2000, 274 (1-3) : 319 - 331
  • [4] Structure of supercooled liquid silicon
    Ansell, S
    Krishnan, S
    Felten, JJ
    Price, DL
    [J]. JOURNAL OF PHYSICS-CONDENSED MATTER, 1998, 10 (03) : L73 - L78
  • [5] X-ray diffraction studies of porous silicon
    Bellet, D
    Dolino, G
    [J]. THIN SOLID FILMS, 1996, 276 (1-2) : 1 - 6
  • [6] Large-scale synthesis of a silicon photonic crystal with a complete three-dimensional bandgap near 1.5 micrometres
    Blanco, A
    Chomski, E
    Grabtchak, S
    Ibisate, M
    John, S
    Leonard, SW
    Lopez, C
    Meseguer, F
    Miguez, H
    Mondia, JP
    Ozin, GA
    Toader, O
    van Driel, HM
    [J]. NATURE, 2000, 405 (6785) : 437 - 440
  • [7] INFRARED VIBRATIONAL-SPECTRA OF AMORPHOUS SI AND GE
    BRODSKY, MH
    LURIO, A
    [J]. PHYSICAL REVIEW B, 1974, 9 (04): : 1646 - 1651
  • [8] COLLINS RT, 1997, PHYS TODAY 0124
  • [9] DEB SK, 1997, ADV HIGH PRESSURE SC, P147
  • [10] CALORIMETRIC STUDIES OF CRYSTALLIZATION AND RELAXATION OF AMORPHOUS SI AND GE PREPARED BY ION-IMPLANTATION
    DONOVAN, EP
    SPAEPEN, F
    TURNBULL, D
    POATE, JM
    JACOBSON, DC
    [J]. JOURNAL OF APPLIED PHYSICS, 1985, 57 (06) : 1795 - 1804