Pressure-induced metallization of silane
- Xiao-Jia Chen*,†,
- Viktor V. Struzhkin*,
- Yang Song*,‡,
- Alexander F. Goncharov*,
- Muhtar Ahart*,
- Zhenxian Liu*,
- Ho-kwang Mao*,§, and
- Russell J. Hemley*,§
- *Geophysical Laboratory, Carnegie Institution of Washington, Washington, DC 20015;
- †School of Physics, South China University of Technology, Guangzhou 510641, China; and
- ‡Department of Chemistry, The University of Western Ontario, London, ON, Canada N6A 5B7
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Contributed by Russell J. Hemley, November 6, 2007 (received for review September 29, 2007)
Abstract
There is a great interest in electronic transitions in hydrogen-rich materials under extreme conditions. It has been recently suggested that the group IVa hydrides such as methane (CH4), silane (SiH4), and germane (GeH4) become metallic at far lower pressures than pure hydrogen at equivalent densities because the hydrogen is chemically compressed in group IVa hydride compounds. Here we report measurements of Raman and infrared spectra of silane under pressure. We find that SiH4 undergoes three phase transitions before becoming opaque at 27–30 GPa. The vibrational spectra indicate the material transforms to a polymeric (framework) structure in this higher pressure range. Room-temperature infrared reflectivity data reveal that the material exhibits Drude-like metallic behavior above 60 GPa, indicating the onset of pressure-induced metallization.
Footnotes
- §To whom correspondence may be addressed. E-mail: h.mao{at}gl.ciw.edu or r.hemley{at}gl.ciw.edu
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Author contributions: X.-J.C., V.V.S., H.-k.M., and R.J.H. designed research; X.-J.C., V.V.S., Y.S., A.F.G., M.A., Z.L., H.-k.M., and R.J.H. performed research; X.-J.C., V.V.S., and A.F.G. analyzed data; and X.-J.C., V.V.S., A.F.G., H.-k.M., and R.J.H. wrote the paper.
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The authors declare no conflict of interest.
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↵ ** The model parameters are: at 60.7 GPa, n d = 2.38, ε∞ = 8.0, γ1 = 384 cm−1, ωp2 = 7.20 × 104 cm−1, ω2 = 6.70 × 103 cm−1, and γ2 = 9.20 × 103 cm−1; at 67.2 GPa, n d = 2.38, ε∞ = 8.0, γ1 = 94.86 cm−1, ωp2=8.36 × 104 cm−1, ω2 = 4.87 × 103 cm−1, and γ2 = 9.19 × 103 cm−1.
- © 2007 by The National Academy of Sciences of the USA





