Structural analysis of the intermetallic surface compound CePt sub(5)/Pt(111)
We report on a detailed low-energy electron diffraction (LEED) and low-temperature scanning tunneling microscopy (STM) study of the intermetallic surface compound CePt sub(5) on Pt(111). Depending on the thickness we observe various diffraction patterns and superstructures. In the low-thickness regi...
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Veröffentlicht in: | Physical review. B, Condensed matter and materials physics Condensed matter and materials physics, 2014-11, Vol.90 (19) |
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creator | Kemmer, Jeannette Praetorius, Christian Kronlein, Andreas Hsu, Pin-Jui Fauth, Kai Bode, Matthias |
description | We report on a detailed low-energy electron diffraction (LEED) and low-temperature scanning tunneling microscopy (STM) study of the intermetallic surface compound CePt sub(5) on Pt(111). Depending on the thickness we observe various diffraction patterns and superstructures. In the low-thickness regime a slightly compressed (2 x 2) superstructure is aligned along the [left angle bracket]110[right angle bracket] direction of the Pt(111) substrate. STM reveals another, much larger superstructure with a periodicity of (9.02 + or - 0.45) nm presumably responsible for the strongly broadened LEED spots. At about 3 unit cells (u.c.) the surface is dominated by a (3[radical]3 x 3[radical]3) R30[degrees] pattern as revealed by LEED satellites and Fourier-transformed high-resolution STM images. It is interpreted as a moire pattern between the film and the substrate. We precisely determine the superstructure of the intermetallic film to ([10/9][radical]3 x [10/9][radical]3) R30[degrees] with respect to the Pt(111) substrate. Above 3 u.c. the satellites progressively disappear. A model is developed that consistently describes this thickness-dependent transition. For CePt sub(5) films with a thickness between 6 and 11 u.c. the lattice of the compressed (2 x 2) superstructure rotates back into the substrate's [left angle bracket]110[right angle bracket] directions. |
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Depending on the thickness we observe various diffraction patterns and superstructures. In the low-thickness regime a slightly compressed (2 x 2) superstructure is aligned along the [left angle bracket]110[right angle bracket] direction of the Pt(111) substrate. STM reveals another, much larger superstructure with a periodicity of (9.02 + or - 0.45) nm presumably responsible for the strongly broadened LEED spots. At about 3 unit cells (u.c.) the surface is dominated by a (3[radical]3 x 3[radical]3) R30[degrees] pattern as revealed by LEED satellites and Fourier-transformed high-resolution STM images. It is interpreted as a moire pattern between the film and the substrate. We precisely determine the superstructure of the intermetallic film to ([10/9][radical]3 x [10/9][radical]3) R30[degrees] with respect to the Pt(111) substrate. Above 3 u.c. the satellites progressively disappear. A model is developed that consistently describes this thickness-dependent transition. 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B, Condensed matter and materials physics</title><description>We report on a detailed low-energy electron diffraction (LEED) and low-temperature scanning tunneling microscopy (STM) study of the intermetallic surface compound CePt sub(5) on Pt(111). Depending on the thickness we observe various diffraction patterns and superstructures. In the low-thickness regime a slightly compressed (2 x 2) superstructure is aligned along the [left angle bracket]110[right angle bracket] direction of the Pt(111) substrate. STM reveals another, much larger superstructure with a periodicity of (9.02 + or - 0.45) nm presumably responsible for the strongly broadened LEED spots. At about 3 unit cells (u.c.) the surface is dominated by a (3[radical]3 x 3[radical]3) R30[degrees] pattern as revealed by LEED satellites and Fourier-transformed high-resolution STM images. It is interpreted as a moire pattern between the film and the substrate. We precisely determine the superstructure of the intermetallic film to ([10/9][radical]3 x [10/9][radical]3) R30[degrees] with respect to the Pt(111) substrate. Above 3 u.c. the satellites progressively disappear. A model is developed that consistently describes this thickness-dependent transition. 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B, Condensed matter and materials physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Kemmer, Jeannette</au><au>Praetorius, Christian</au><au>Kronlein, Andreas</au><au>Hsu, Pin-Jui</au><au>Fauth, Kai</au><au>Bode, Matthias</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Structural analysis of the intermetallic surface compound CePt sub(5)/Pt(111)</atitle><jtitle>Physical review. B, Condensed matter and materials physics</jtitle><date>2014-11-15</date><risdate>2014</risdate><volume>90</volume><issue>19</issue><issn>1098-0121</issn><eissn>1550-235X</eissn><abstract>We report on a detailed low-energy electron diffraction (LEED) and low-temperature scanning tunneling microscopy (STM) study of the intermetallic surface compound CePt sub(5) on Pt(111). Depending on the thickness we observe various diffraction patterns and superstructures. In the low-thickness regime a slightly compressed (2 x 2) superstructure is aligned along the [left angle bracket]110[right angle bracket] direction of the Pt(111) substrate. STM reveals another, much larger superstructure with a periodicity of (9.02 + or - 0.45) nm presumably responsible for the strongly broadened LEED spots. At about 3 unit cells (u.c.) the surface is dominated by a (3[radical]3 x 3[radical]3) R30[degrees] pattern as revealed by LEED satellites and Fourier-transformed high-resolution STM images. It is interpreted as a moire pattern between the film and the substrate. We precisely determine the superstructure of the intermetallic film to ([10/9][radical]3 x [10/9][radical]3) R30[degrees] with respect to the Pt(111) substrate. Above 3 u.c. the satellites progressively disappear. A model is developed that consistently describes this thickness-dependent transition. For CePt sub(5) films with a thickness between 6 and 11 u.c. the lattice of the compressed (2 x 2) superstructure rotates back into the substrate's [left angle bracket]110[right angle bracket] directions.</abstract></addata></record> |
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subjects | Brackets Compressed Condensed matter Intermetallics Mathematical models Satellite imagery Scanning tunneling microscopy Superstructures Unit cell |
title | Structural analysis of the intermetallic surface compound CePt sub(5)/Pt(111) |
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