Результаты исследований: Научные публикации в периодических изданиях › статья › Рецензирование
Reconstruction phase transition c(4×4) – (1×3) on the (001)InSb surface. / Bakarov, A.; Galitsyn, Yu; Mansurov, V. и др.
в: Journal of Crystal Growth, Том 457, 01.01.2017, стр. 207-210.Результаты исследований: Научные публикации в периодических изданиях › статья › Рецензирование
}
TY - JOUR
T1 - Reconstruction phase transition c(4×4) – (1×3) on the (001)InSb surface
AU - Bakarov, A.
AU - Galitsyn, Yu
AU - Mansurov, V.
AU - Zhuravlev, K.
N1 - Publisher Copyright: © 2016 Elsevier B.V.
PY - 2017/1/1
Y1 - 2017/1/1
N2 - The (001) surface of InSb is the most common growth surface, forming a number of surface reconstructions depending on the both ratio of group III and V species presented on surface and substrate temperature. In the present work surface structures were studied using reflection high energy electron diffraction (RHEED). The c(4×4)↔(1×3) reconstruction transition was investigated in details. The intensity of fractional spots of c(4×4) structure was measured during the variation of antimony flux at different substrate temperatures. At the substrate temperatures of T<400 °C, hysteresis loop of fractional spot intensity appeared during the forward and reverse Sb flux variation, testifying that c(4×4)↔(1×3) transition is discontinuous first order phase transition. At the temperatures T>400 °C, hysteresis loop was not observed, that corresponds to continuous phase transition. It was shown that phase transition is analogous to the van der Waals transition. We developed a model to describe c(4×4)↔(1×3) transition in the framework of the lattice gas approximation. This model takes into account the complex nature of indirect interactions that result in the effective attraction between lattice gas cells forming surface reconstruction. The calculated surface state isotherms are in a good agreement with the experimental isotherms.
AB - The (001) surface of InSb is the most common growth surface, forming a number of surface reconstructions depending on the both ratio of group III and V species presented on surface and substrate temperature. In the present work surface structures were studied using reflection high energy electron diffraction (RHEED). The c(4×4)↔(1×3) reconstruction transition was investigated in details. The intensity of fractional spots of c(4×4) structure was measured during the variation of antimony flux at different substrate temperatures. At the substrate temperatures of T<400 °C, hysteresis loop of fractional spot intensity appeared during the forward and reverse Sb flux variation, testifying that c(4×4)↔(1×3) transition is discontinuous first order phase transition. At the temperatures T>400 °C, hysteresis loop was not observed, that corresponds to continuous phase transition. It was shown that phase transition is analogous to the van der Waals transition. We developed a model to describe c(4×4)↔(1×3) transition in the framework of the lattice gas approximation. This model takes into account the complex nature of indirect interactions that result in the effective attraction between lattice gas cells forming surface reconstruction. The calculated surface state isotherms are in a good agreement with the experimental isotherms.
KW - A1. Phase transition
KW - A1. Reflection high energy electron diffraction
KW - A1. Surface structure
KW - B1. InSb
KW - INSB(001)
KW - INSB(100)
KW - MOLECULAR-BEAM EPITAXY
KW - RHEED
KW - Surface structure
KW - SB
KW - Reflection high energy electron diffraction
KW - InSb
KW - INSB
KW - GROWTH
KW - Phase transition
UR - http://www.scopus.com/inward/record.url?scp=84964653578&partnerID=8YFLogxK
U2 - 10.1016/j.jcrysgro.2016.04.051
DO - 10.1016/j.jcrysgro.2016.04.051
M3 - Article
AN - SCOPUS:84964653578
VL - 457
SP - 207
EP - 210
JO - Journal of Crystal Growth
JF - Journal of Crystal Growth
SN - 0022-0248
ER -
ID: 9562199