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Adsorbate induced mesoscopic surface reconstruction of the system Te/Pd(102)

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OriginalspracheEnglisch
Seiten (von - bis)126-134
Seitenumfang9
FachzeitschriftSurface Science
Jahrgang489
Ausgabenummer1-3
PublikationsstatusVeröffentlicht - 20 Aug. 2001

Abstract

Low energy electron diffraction (LEED) measurements have been carried out on the clean and Te covered Pd(102) surface. This is the surface into which the Pd(100) surface is reconstructed by a concentration of more than 0.5 ML of Te. The Pd(102) surface was produced with a terrace width of more than 1000 Å. Up to 0.5 ML the adsorption of Te takes place on the flat (102) surface, on which islands with (2 × 1) structure are formed coupled with a reduction of the terrace widths to about half the initial value. Above 0.5 ML, and up to 1 ML, the adsorbed Te atoms produce a structural change of the surface, i.e. a terrace structure is formed with a clear average terrace length that depends on Te concentration and with step edges in [2̄01] direction. As concluded from the characteristic splitting of LEED spots as a function of energy, these terraces occupy only two height levels in an alternating sequence and are separated by steps of single atomic height. The terrace width of the alternating te rraces increases with increasing Te-concentration. Again a flat surface is formed at 1 ML of Te. A geometrical model is established and discussed.

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Adsorbate induced mesoscopic surface reconstruction of the system Te/Pd(102). / Godzik, G.; Pfnür, Herbert.
in: Surface Science, Jahrgang 489, Nr. 1-3, 20.08.2001, S. 126-134.

Publikation: Beitrag in FachzeitschriftArtikelForschungPeer-Review

Godzik G, Pfnür H. Adsorbate induced mesoscopic surface reconstruction of the system Te/Pd(102). Surface Science. 2001 Aug 20;489(1-3):126-134. doi: 10.1016/S0039-6028(01)01170-0
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abstract = "Low energy electron diffraction (LEED) measurements have been carried out on the clean and Te covered Pd(102) surface. This is the surface into which the Pd(100) surface is reconstructed by a concentration of more than 0.5 ML of Te. The Pd(102) surface was produced with a terrace width of more than 1000 {\AA}. Up to 0.5 ML the adsorption of Te takes place on the flat (102) surface, on which islands with (2 × 1) structure are formed coupled with a reduction of the terrace widths to about half the initial value. Above 0.5 ML, and up to 1 ML, the adsorbed Te atoms produce a structural change of the surface, i.e. a terrace structure is formed with a clear average terrace length that depends on Te concentration and with step edges in [{\=2}01] direction. As concluded from the characteristic splitting of LEED spots as a function of energy, these terraces occupy only two height levels in an alternating sequence and are separated by steps of single atomic height. The terrace width of the alternating te rraces increases with increasing Te-concentration. Again a flat surface is formed at 1 ML of Te. A geometrical model is established and discussed.",
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AU - Godzik, G.

AU - Pfnür, Herbert

N1 - Funding information: This work was supported by the Deutsche Forschungsgemeinschaft. Stimulating discussions with I. Vilfan are gratefully acknowledged.

PY - 2001/8/20

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N2 - Low energy electron diffraction (LEED) measurements have been carried out on the clean and Te covered Pd(102) surface. This is the surface into which the Pd(100) surface is reconstructed by a concentration of more than 0.5 ML of Te. The Pd(102) surface was produced with a terrace width of more than 1000 Å. Up to 0.5 ML the adsorption of Te takes place on the flat (102) surface, on which islands with (2 × 1) structure are formed coupled with a reduction of the terrace widths to about half the initial value. Above 0.5 ML, and up to 1 ML, the adsorbed Te atoms produce a structural change of the surface, i.e. a terrace structure is formed with a clear average terrace length that depends on Te concentration and with step edges in [2̄01] direction. As concluded from the characteristic splitting of LEED spots as a function of energy, these terraces occupy only two height levels in an alternating sequence and are separated by steps of single atomic height. The terrace width of the alternating te rraces increases with increasing Te-concentration. Again a flat surface is formed at 1 ML of Te. A geometrical model is established and discussed.

AB - Low energy electron diffraction (LEED) measurements have been carried out on the clean and Te covered Pd(102) surface. This is the surface into which the Pd(100) surface is reconstructed by a concentration of more than 0.5 ML of Te. The Pd(102) surface was produced with a terrace width of more than 1000 Å. Up to 0.5 ML the adsorption of Te takes place on the flat (102) surface, on which islands with (2 × 1) structure are formed coupled with a reduction of the terrace widths to about half the initial value. Above 0.5 ML, and up to 1 ML, the adsorbed Te atoms produce a structural change of the surface, i.e. a terrace structure is formed with a clear average terrace length that depends on Te concentration and with step edges in [2̄01] direction. As concluded from the characteristic splitting of LEED spots as a function of energy, these terraces occupy only two height levels in an alternating sequence and are separated by steps of single atomic height. The terrace width of the alternating te rraces increases with increasing Te-concentration. Again a flat surface is formed at 1 ML of Te. A geometrical model is established and discussed.

KW - Adatoms

KW - Low energy electron diffraction (LEED)

KW - Palladium

KW - Surface relaxation and reconstruction

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U2 - 10.1016/S0039-6028(01)01170-0

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JO - Surface Science

JF - Surface Science

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