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$\mathsf{\sqrt{3}}$ linear structures in the Te/Ni(111) system
Authors:Email author" target="_blank">S?SueharaEmail author  T?Aizawa  S?Hishita  A?Nukui  S?Inoue
Institution:(1) Advanced Materials Laboratory, National Institute for Materials Science, 1-1 Namiki, 305-0044 Tsukuba, Ibaraki, Japan
Abstract:Surface structures in the Te/Ni(111) system are revealed by using reflection high-energy electron diffraction combined with X-ray and ultraviolet photoelectron spectroscopies. At a 0.33 mono-layer (ML)-Te/Ni(111) surface, a reversible structural phase transition is observed with a transition temperature Tc of 380 $^{\circ}$ C. The diffraction pattern from the low temperature phase is accompanied by streaks. The high and low temperature phases are characterized by $\sqrt{3} \times \sqrt{3} R\pm30^{\circ}$ and $3 \times \sqrt{3}$ rectangle, respectively. The mechanism of the phase transition is explained by the order-disorder transition with a rumpled chain model. Both 0.51 ML- and 0.44 ML-Te/Ni(111) surfaces exhibit the complex diffraction patterns accompanied by diffuse streaks. These surface structures are characterized by the $7 \times \sqrt{3}$ rectangle and $5 \sqrt{3} \times \sqrt{3} R \pm30^{\circ}$ , respectively. All diffuse streaks obtained at the above surfaces are consistently interpreted in the view of the ill-ordered arrangements of the well-ordered $\sqrt{3}$ linear chains. It is shown that the ldquo $\sqrt{3}$ linear structurerdquo is the key in the Te/Ni(111) system.Received: 1 December 2003, Published online: 20 April 2004PACS: 61.14.Hg Low-energy electron diffraction (LEED) and reflection high-energy electron diffraction (RHEED) - 68.65.-k Low-dimensional, mesoscopic, and nanoscale systems: structure and nonelectronic properties - 64.60.Cn Order-disorder transformations; statistical mechanics of model systems
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