Gerald Lucovsky and James C Phillips 2007 J. Phys.: Condens. Matter 19 455219 doi:10.1088/0953-8984/19/45/455219
Gerald Lucovsky1 and James C Phillips2
Show affiliationsRecent research results have suggested that double percolation processes play a significant role in the formation of intermediate phases (IPs) in non-crystalline thin films. One class of IP windows, involving competitive double percolation, occurs in binary AsxSe1−x and GexSe1−x alloys and in the pseudo-binary AsxGexSe1−2x alloy. This IP window occurs over an 8–12% composition range. Transitions that define the IP window in the Ge–Se alloys involve a competition between the elimination of compliant local bonding dimer groups, e.g. Ge–Se–Se–Ge, at the expense of an increasing fraction of rigid local bonding monomer groups, e.g. Ge–Se–Ge. Compliant monomer group bonding defines the first window transition for an average number of bonding constraints/atom, nc = 3; the second transition from rigid to stressed rigid occurs when the compliant monomer concentration drops below a concentration for percolation. A second class of IPs with significantly narrower composition windows, ~1 to at most 3%, is proposed to explain experimentally determined IPs in chalcogenide alloys with halogen dopants; e.g. a-Ge0.25Se0.77−xIx, where the IP window width is ~1%. We suggest that this narrow window is determined by a confluent coherent double percolation process that includes (i) broken bond-bending constraints that minimize local bond strain, and (ii) a percolation pathway based on a second and complementary local bonding group. However, this second class of IPs is not supported by theory and modeling as yet, and as such our designation of this class of IPs must be regarded as more speculative. On the other had, it is significant that at least two other alloy systems, Ge2Se2Te5 and pseudo-ternary Hf, Zr and Ti Si oxynitrides, display narrow regimes where bond constraint counting indicates local strain suppression, and where a second and larger bonding arrangement is present at the percolation limit.
68.55.Nq Composition and phase identification
64.60.A- Specific approaches applied to studies of phase transitions
68.55.Ln Defects and impurities: doping, implantation, distribution, concentration, etc.
Issue 45 (14 November 2007)
Received 13 September 2007
Published 24 October 2007
Gerald Lucovsky and James C Phillips 2007 J. Phys.: Condens. Matter 19 455219
Iddo Eliazar and Joseph Klafter 2008 J. Phys. A: Math. Theor. 41 122001
Fang Jian-Hui et al 2009 Chinese Phys. Lett. 26 110202
Jinlong Zhang et al 2008 J. Micromech. Microeng. 18 125025
Sonia L'Innocente et al 2009 J. Phys. A: Math. Theor. 42 475305
Xue-Chai Chen et al 2008 Nanotechnology 19 235105
Magnus Rattray et al 2009 J. Phys.: Conf. Ser. 197 012002
E G Thorsteinsson and J T Gudmundsson 2010 Plasma Sources Sci. Technol. 19 015001
T Abe et al 2009 J. Phys.: Conf. Ser. 191 012023
E A Brener et al 2009 J. Phys.: Condens. Matter 21 464106