Details
Original language | English |
---|---|
Pages (from-to) | 229-242 |
Number of pages | 14 |
Journal | Surface Science |
Volume | 460 |
Issue number | 1-3 |
Publication status | Published - 20 Jul 2000 |
Abstract
Ordered phases of Sr on Mo(112) and their phase transitions have been studied up to one physical monolayer as a function of both coverage and temperature using optical LEED. Starting at a coverage of 0.07, islands of a p(8 × 1) structure are formed at 100 K, which coexist with a disordered lattice gas. The formation of incommensurate structures with properties of floating solids starts already at coverages slightly above the completed p(8 × 1) commensurate structure (θ=0.125). The latter itself behaves like a floating solid and undergoes a depinning transition at T ≈ 125 K, similar to the next commensurate structure, p(5 × 1), which is formed at θ=0.20. Floating solids are found in the whole coverage range between 0.12 and 0.23. At higher coverage coexistence between p(5 × 1) and c(2 × 2) structures is found, which melt by forming intermediate two-dimensional eutectics, i.e. coexistence regions with their melts, with an eutectic point at θ=0.37, Teu = 310 K. Close to a coverage of 0.5 a homogenous phase is formed, which disorders by a continuous phase transition, as explicitly tested by determination of the critical exponents β of the order parameter and ν of the correlation length. It is shown that the system belongs to the universality class of the Ising model. An incommensurate phase is again formed at higher coverage due to uniaxial compression of the layers. The behaviour at low coverages can be qualitatively understood assuming lateral interactions along the furrows mainly caused by dipole-dipole interactions and electrostatic screening of the adsorbate induced charge redistribution.
Keywords
- Low energy electron diffraction, Molybdenum, Phase transitions, Strontium
ASJC Scopus subject areas
- Physics and Astronomy(all)
- Condensed Matter Physics
- Physics and Astronomy(all)
- Surfaces and Interfaces
- Materials Science(all)
- Surfaces, Coatings and Films
- Materials Science(all)
- Materials Chemistry
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In: Surface Science, Vol. 460, No. 1-3, 20.07.2000, p. 229-242.
Research output: Contribution to journal › Article › Research › peer review
}
TY - JOUR
T1 - Phase transitions in two-dimensional anisotropic chain systems
T2 - Submonolayers of Sr adsorbed on Mo(112)
AU - Fedorus, A.
AU - Godzik, G.
AU - Koval, V.
AU - Naumovets, A.
AU - Pfnür, Herbert
N1 - Funding information: We thank I. Lyuksyutov for helpful discussions. Support by the Volkswagen-Stiftung and by the Deutsche Forschungsgemeinschaft is gratefully acknowledged.
PY - 2000/7/20
Y1 - 2000/7/20
N2 - Ordered phases of Sr on Mo(112) and their phase transitions have been studied up to one physical monolayer as a function of both coverage and temperature using optical LEED. Starting at a coverage of 0.07, islands of a p(8 × 1) structure are formed at 100 K, which coexist with a disordered lattice gas. The formation of incommensurate structures with properties of floating solids starts already at coverages slightly above the completed p(8 × 1) commensurate structure (θ=0.125). The latter itself behaves like a floating solid and undergoes a depinning transition at T ≈ 125 K, similar to the next commensurate structure, p(5 × 1), which is formed at θ=0.20. Floating solids are found in the whole coverage range between 0.12 and 0.23. At higher coverage coexistence between p(5 × 1) and c(2 × 2) structures is found, which melt by forming intermediate two-dimensional eutectics, i.e. coexistence regions with their melts, with an eutectic point at θ=0.37, Teu = 310 K. Close to a coverage of 0.5 a homogenous phase is formed, which disorders by a continuous phase transition, as explicitly tested by determination of the critical exponents β of the order parameter and ν of the correlation length. It is shown that the system belongs to the universality class of the Ising model. An incommensurate phase is again formed at higher coverage due to uniaxial compression of the layers. The behaviour at low coverages can be qualitatively understood assuming lateral interactions along the furrows mainly caused by dipole-dipole interactions and electrostatic screening of the adsorbate induced charge redistribution.
AB - Ordered phases of Sr on Mo(112) and their phase transitions have been studied up to one physical monolayer as a function of both coverage and temperature using optical LEED. Starting at a coverage of 0.07, islands of a p(8 × 1) structure are formed at 100 K, which coexist with a disordered lattice gas. The formation of incommensurate structures with properties of floating solids starts already at coverages slightly above the completed p(8 × 1) commensurate structure (θ=0.125). The latter itself behaves like a floating solid and undergoes a depinning transition at T ≈ 125 K, similar to the next commensurate structure, p(5 × 1), which is formed at θ=0.20. Floating solids are found in the whole coverage range between 0.12 and 0.23. At higher coverage coexistence between p(5 × 1) and c(2 × 2) structures is found, which melt by forming intermediate two-dimensional eutectics, i.e. coexistence regions with their melts, with an eutectic point at θ=0.37, Teu = 310 K. Close to a coverage of 0.5 a homogenous phase is formed, which disorders by a continuous phase transition, as explicitly tested by determination of the critical exponents β of the order parameter and ν of the correlation length. It is shown that the system belongs to the universality class of the Ising model. An incommensurate phase is again formed at higher coverage due to uniaxial compression of the layers. The behaviour at low coverages can be qualitatively understood assuming lateral interactions along the furrows mainly caused by dipole-dipole interactions and electrostatic screening of the adsorbate induced charge redistribution.
KW - Low energy electron diffraction
KW - Molybdenum
KW - Phase transitions
KW - Strontium
UR - http://www.scopus.com/inward/record.url?scp=0000824595&partnerID=8YFLogxK
U2 - 10.1016/S0039-6028(00)00545-8
DO - 10.1016/S0039-6028(00)00545-8
M3 - Article
AN - SCOPUS:0000824595
VL - 460
SP - 229
EP - 242
JO - Surface Science
JF - Surface Science
SN - 0039-6028
IS - 1-3
ER -