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Auteur : Grafiati
Publié le 11 mars 2023

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1

Wasielewski, R., M. Grodzicki, J. Sito, K. Lament, P. Mazur et A. Ciszewski. « Ru/GaN(0001) Interface Properties ». Acta Physica Polonica A 132, no 2 (août 2017) : 354–57. http://dx.doi.org/10.12693/aphyspola.132.354.

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2

GODOWSKI, P. J., Z. S. LI, J. BORK et J. ONSGAARD. « STUDY OF THE Pt/Ru(0001) INTERFACE ». Surface Review and Letters 14, no 05 (octobre 2007) : 911–14. http://dx.doi.org/10.1142/s0218625x07010378.

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The growth process of platinum on Ru (0001) near room temperature was characterized using photoelectron spectroscopy of high resolution. The binding energy position and intensity of the Pt 4f7/2 and Ru 3d5/2 core levels as well as the shape and structure of the valence band spectra corresponding to the different stages of the deposition were analyzed. Up to ca. two adsorbate monolayers, the intensity changes of the peaks indicated layer-by-layer growth mode. The surface core level shifts of Ru and Pt levels were evaluated as -0.33 and -0.476 eV, respectively. The valence band spectra show a rather weak interaction between the d-bands of Pt and Ru .
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3

Wang, Changqing, Weiguang Chen et Jingpei Xie. « Effects of Transition Element Additions on the Interfacial Interaction and Electronic Structure of Al(111)/6H-SiC(0001) Interface : A First-Principles Study ». Materials 14, no 3 (29 janvier 2021) : 630. http://dx.doi.org/10.3390/ma14030630.

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In this work, the effects of 20 transition element additions on the interfacial adhesion energy and electronic structure of Al(111)/6H-SiC(0001) interfaces have been studied by the first-principles method. For pristine Al(111)/6H-SiC(0001) interfaces, both Si-terminated and C-terminated interfaces have covalent bond characteristics. The C-terminated interface has higher binding energy, which is mainly due to the stronger covalent bond formed by the larger charge transfer between C and Al. The results show that the introduction of many transition elements, such as 3d transitional group Mn, Fe, Co, Ni, Cu, Zn and 4d transitional group Tc, Ru, Rh, Pd, Ag, can improve the interfacial adhesion energy of the Si-terminated Al(111)/6H-SiC(0001) interface. However, for the C-terminated Al(111)/6H-SiC(0001) interface, only the addition of Co element can improve the interfacial adhesion energy. Bader charge analysis shows that the increase of interfacial binding energy is mainly attributed to more charge transfer.
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Tollefsen, H., E. O. Laastad, X. Yu et S. Raaen. « Initial oxidation of the Ce–Ru(0001) interface ». Philosophical Magazine 88, no 5 (11 février 2008) : 665–75. http://dx.doi.org/10.1080/14786430801946625.

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PROKOP, J., M. PRZYBYLSKI, T. SLEZAK et J. KORECKI. « NONMAGNETIC IRON LAYERS AT THE Fe/Ru INTERFACE ». Surface Review and Letters 04, no 06 (décembre 1997) : 1239–43. http://dx.doi.org/10.1142/s0218625x97001607.

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Magnetic dead layers near the Fe/Ru interface in iron films grown on Ru(0001) and in Fe/Ru multilayers have been reported previously. In this paper the CEMS analysis is applied to explain why these interfacial Fe atoms are nonmagnetic. The CEMS spectra of the uncoated bcc-Fe surface clearly show the ferromagnetic order. After covering with ruthenium, the characteristic changes in the conversion electron Mössbauer spectrum were observed, which indicate existence of a nonferromagnetic phase near the Fe/Ru interface. The measured value of the isomer shift of the interface component suggests that the bcc phase persists after covering of the Fe film with Ru.
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6

ANDERSEN, T. H., L. BECH, J. ONSGAARD, S. V. HOFFMANN et Z. LI. « HIGH RESOLUTION CORE LEVEL SPECTROSCOPY AT THE Cu/Ru(0001) INTERFACE ». Surface Review and Letters 09, no 02 (avril 2002) : 723–27. http://dx.doi.org/10.1142/s0218625x02002798.

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Copper adsorption on Ru(0001) has been studied by synchrotron radiation. The clean Ru 3d 5/2 spectra were found to consist of two components with a binding energy shift of 400 meV. The component with the lower binding energy represents the first layer of ruthenium atoms. Adsorption of copper gives rise to core level shifts of the Ru 3d 5/2 components, which were studied as a function of Cu coverage. Experiments were carried out with copper coverages varying from the submonolayer range up to two monolayers of copper. The binding energy of the Cu 2p 3/2 level was measured by X-ray photoemission spectroscopy.
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7

Jiang, De-en, Mao-Hua Du et Sheng Dai. « First principles study of the graphene/Ru(0001) interface ». Journal of Chemical Physics 130, no 7 (21 février 2009) : 074705. http://dx.doi.org/10.1063/1.3077295.

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Wang, Miao, Gang Liu, Min Huang, Yabo Fu, Changhong Lin, Jianbo Wu et Vladimir A. Levchenko. « Investigation of the Adhesion Strength, Fracture Toughness, and Stability of M/Cr2N and M/V2N (M = Ti, Ru, Ni, Pd, Al, Ag, and Cu) Interfaces Based on First-Principles Calculations ». Coatings 12, no 1 (7 janvier 2022) : 66. http://dx.doi.org/10.3390/coatings12010066.

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Obtaining detailed information regarding the interfacial characteristics of metal/hexagonal-TMN composites is imperative for developing these materials with optimal mechanical properties. To this end, we systematically investigate the work of adhesion, fracture toughness, and interfacial stability of M/Cr2N and M/V2N interfaces using first-principles calculations. The orientation (0001) of hexagonal phases and (111) of fcc phases are selected as the interface orientations. Accordingly, we construct M/Cr2N interface models by considering 1N, 2N, and Cr terminations of Cr2N(0001), as well as two stacking sequences (top and hollow sites) for the 1N- and 2N-terminated interface models, respectively. The M/V2N interface models are constructed in the same way. The V-terminated Ni/V2N interface is demonstrated to provide a good combination of the work of adhesion, fracture toughness, and interfacial stability. Therefore, the Ni/V2N interface model can be regarded as the preferred configuration among the metal/hexagonal-TMN interface models considered. The present results offer a practical perspective for tailoring the interfaces in metal/hexagonal-TMN composite materials to obtain improved mechanical properties.
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9

Godowski, P. J., J. Onsgaard, Z. Ryszka, Ł. Rok et Zhe Shen Li. « Phase transformations of the Pt/Ru(0001) interface studied by photoemission ». Surface Science 602, no 2 (janvier 2008) : 465–69. http://dx.doi.org/10.1016/j.susc.2007.10.038.

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Houston, J. E., J. M. White, P. J. Feibelman et D. R. Hamann. « Interface-state properties for strained-layer Ni adsorbed on Ru(0001) ». Physical Review B 38, no 17 (15 décembre 1988) : 12164–70. http://dx.doi.org/10.1103/physrevb.38.12164.

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11

Jin, Li, Qiang Fu, Yang Yang et Xinhe Bao. « A comparative study of intercalation mechanism at graphene/Ru(0001) interface ». Surface Science 617 (novembre 2013) : 81–86. http://dx.doi.org/10.1016/j.susc.2013.07.008.

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12

Godowski, P. J., J. Onsgaard et Z. S. Li. « CO-Induced Photoemission Structures of the CO/Pt/Ru(0001) Interface ». Acta Physica Polonica A 130, no 6 (décembre 2016) : 1389–94. http://dx.doi.org/10.12693/aphyspola.130.1389.

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Cored, Jorge, Mengen Wang, Nusnin Akter, Zubin Darbari, Yixin Xu, Burcu Karagoz, Iradwikanari Waluyo et al. « Water Formation Reaction under Interfacial Confinement : Al0.25Si0.75O2 on O-Ru(0001) ». Nanomaterials 12, no 2 (6 janvier 2022) : 183. http://dx.doi.org/10.3390/nano12020183.

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Confined nanosized spaces at the interface between a metal and a seemingly inert material, such as a silicate, have recently been shown to influence the chemistry at the metal surface. In prior work, we observed that a bilayer (BL) silica on Ru(0001) can change the reaction pathway of the water formation reaction (WFR) near room temperature when compared to the bare metal. In this work, we looked at the effect of doping the silicate with Al, resulting in a stoichiometry of Al0.25Si0.75O2. We investigated the kinetics of WFR at elevated H2 pressures and various temperatures under interfacial confinement using ambient pressure X-ray photoelectron spectroscopy. The apparent activation energy was lower than that on bare Ru(0001) but higher than that on the BL-silica/Ru(0001). The apparent reaction order with respect to H2 was also determined. The increased residence time of water at the surface, resulting from the presence of the BL-aluminosilicate (and its subsequent electrostatic stabilization), favors the so-called disproportionation reaction pathway (*H2O + *O ↔ 2 *OH), but with a higher energy barrier than for pure BL-silica.
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14

Shin, Jinhyun, Astini Vita, Sari Windu, Jung-Hae Choi, Seung-Cheol Lee et June Gunn Lee. « Energetics and Interdiffusion at the Cu/Ru(0001) Interface : Density Functional Calculations ». Journal of Nanoscience and Nanotechnology 11, no 7 (1 juillet 2011) : 6589–93. http://dx.doi.org/10.1166/jnn.2011.4460.

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15

Pötschke, G. O., et R. J. Behm. « Interface structure and misfit dislocations in thin Cu films on Ru(0001) ». Physical Review B 44, no 3 (15 juillet 1991) : 1442–45. http://dx.doi.org/10.1103/physrevb.44.1442.

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16

Wu Yue, Huang Han, Mao Hong-Ying, Yang Xin-Guo, Zhang Jian-Hua, Wang Mang, Li Hai-Yang, He Pi-Mo et Bao Shi-Ning. « Study on the interface of an organic semiconductor grown on Ru(0001) surface ». Acta Physica Sinica 53, no 5 (2004) : 1604. http://dx.doi.org/10.7498/aps.53.1604.

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17

Mougel, Loic, Patrick M. Buhl, Qili Li, Anika Müller, Hung-Hsiang Yang, Matthieu J. Verstraete, Pascal Simon, Bertrand Dupé et Wulf Wulfhekel. « Strong effect of crystal structure on the proximity effect between a superconductor and monolayer of cobalt ». Applied Physics Letters 121, no 23 (5 décembre 2022) : 231605. http://dx.doi.org/10.1063/5.0130313.

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We present an unexpectedly strong influence of the proximity effect between the bulk Ru(0001) superconductor and atomically thin layers of Co on the crystal structure of the latter. The Co monolayer grows in two different modifications, such as hcp stacking and a reconstructed ε-like phase. While hcp islands show a weak proximity effect on Co and a little suppression of superconductivity in the substrate next to it, the more complex ε-like stacking becomes almost fully superconducting. We explain the weak proximity effect between Ru and hcp Co and the rather abrupt jump of the superconducting order parameter by a low transparency of the interface. In contrast, the strong proximity effect without a jump of the order parameter in the ε-like phase indicates a highly transparent interface. This work highlights that the proximity effect between a superconductor and a normal metal strongly depends on the crystal structure of the interface, which allows to engineer the proximity effect in hybrid structures.
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18

AZIZI, A., J. ARABSKI et A. DINIA. « GROWTH, MORPHOLOGICAL AND STRUCTURAL PROPERTIES OF Ag THIN FILMS ON A Ru (0001) SURFACE GROWN BY MBE ». Surface Review and Letters 11, no 06 (décembre 2004) : 563–68. http://dx.doi.org/10.1142/s0218625x04006517.

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Ag thin films deposited on Ru (0001) surface by molecular beam epitaxy, at temperatures of 20°C and 450°C, have been investigated using reflection high-energy electron diffraction (RHEED), atomic force microscopy (AFM) and X-ray diffraction (XRD) techniques. For both growth temperatures, the in situ RHEED patterns of the Ag films exhibited an in-plane six-fold symmetry, indicating that the Ag deposit is in epitaxy with the Ru buffer surface. At RT, the RHEED technique indicated a three-dimensional growth (3D), while a layer-by-layer growth (2D) takes place at HT. The AFM images showed a granular structure of the surface of the deposited Ag layers with a large variation of the roughness with the growth temperature. XRD analysis gave indication of a strongly textured thin film along the growth direction. The lattice mismatch between the Ag and Ru is at the origin of a stress at the interface and defects structure in the film.
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19

Houston, J. E., C. H. F. Peden, Peter J. Feibelman et D. R. Hamann. « Observation of a true interface state in strained-layer Cu adsorption on Ru(0001) ». Physical Review Letters 56, no 4 (27 janvier 1986) : 375–77. http://dx.doi.org/10.1103/physrevlett.56.375.

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20

Zhong, Jian-Qiang, Mengen Wang, Nusnin Akter, Dario J. Stacchiola, Deyu Lu et J. Anibal Boscoboinik. « Room-Temperature in Vacuo Chemisorption of Xenon Atoms on Ru(0001) under Interface Confinement ». Journal of Physical Chemistry C 123, no 22 (26 avril 2019) : 13578–85. http://dx.doi.org/10.1021/acs.jpcc.9b01110.

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21

Wang, Mengen, Jian-Qiang Zhong, Dario J. Stacchiola, J. Anibal Boscoboinik et Deyu Lu. « First-Principles Study of Interface Structures and Charge Rearrangement at the Aluminosilicate/Ru(0001) Heterojunction ». Journal of Physical Chemistry C 123, no 13 (9 septembre 2018) : 7731–39. http://dx.doi.org/10.1021/acs.jpcc.8b05853.

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Wang, Mengen, Jian-Qiang Zhong, John Kestell, Iradwikanari Waluyo, Dario J. Stacchiola, J. Anibal Boscoboinik et Deyu Lu. « Energy Level Shifts at the Silica/Ru(0001) Heterojunction Driven by Surface and Interface Dipoles ». Topics in Catalysis 60, no 6-7 (12 septembre 2016) : 481–91. http://dx.doi.org/10.1007/s11244-016-0704-x.

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23

Süle, P., et M. Szendrő. « The classical molecular dynamics simulation of graphene on Ru(0001) using a fitted Tersoff interface potential ». Surface and Interface Analysis 46, no 1 (4 novembre 2013) : 42–47. http://dx.doi.org/10.1002/sia.5344.

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Huang, Li, Yi Pan, Lida Pan, Min Gao, Wenyan Xu, Yande Que, Haitao Zhou, Yeliang Wang, Shixuan Du et H. J. Gao. « Intercalation of metal islands and films at the interface of epitaxially grown graphene and Ru(0001) surfaces ». Applied Physics Letters 99, no 16 (17 octobre 2011) : 163107. http://dx.doi.org/10.1063/1.3653241.

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Dhar, Bijoya, Joshua Pollock, Jillian Gloria et William E. Kaden. « TPD characterization of Al-OD-Si sites at the interface of bilayer Al0.42Si0.58O2/Ru(0001) thin-films. » Surface Science 696 (juin 2020) : 121595. http://dx.doi.org/10.1016/j.susc.2020.121595.

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Houston, J. E., C. H. F. Peden, P. J. Feibelman et D. R. Hamann. « Summary Abstract : Studies of the interaction of CO with the interface states for strained‐layer Cu on Ru(0001) ». Journal of Vacuum Science & ; Technology A : Vacuum, Surfaces, and Films 5, no 4 (juillet 1987) : 688–89. http://dx.doi.org/10.1116/1.574377.

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Badyal, Jas Pal S., Andrew J. Gellman, Robert W. Judd et Richard M. Lambert. « Single crystal modelling of the SMSI phenomenon : Structure, composition, electronic effects and CO chemisorption at the Ru(0001)/TiOx interface ». Catalysis Letters 1, no 1-3 (1988) : 41–50. http://dx.doi.org/10.1007/bf00765352.

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WALKER, A. P., et R. M. LAMBERT. « ChemInform Abstract : Properties of the Ru(0001)/Ce-H2 Interface : A Model System for Transition-Metal/Rare-Earth Hydride Catalysts. » ChemInform 23, no 22 (22 août 2010) : no. http://dx.doi.org/10.1002/chin.199222019.

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Andersen, T. H., Z. Li, S. V. Hoffmann, L. Bech et J. Onsgaard. « Photoelectron spectroscopy studies of the Pd/Ru(0001) and (Cu Pd)/Ru(0001) interfaces ». Journal of Physics : Condensed Matter 14, no 34 (22 août 2002) : 7853–64. http://dx.doi.org/10.1088/0953-8984/14/34/305.

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Prieto, J. E., E. M. Trapero, P. Prieto, E. García-Martín, G. D. Soria, P. Galán et J. de la Figuera. « RBS/Channeling characterization of Ru(0001) and thin epitaxial Ru/Al2O3(0001) films ». Applied Surface Science 582 (avril 2022) : 152304. http://dx.doi.org/10.1016/j.apsusc.2021.152304.

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31

OVER, H., H. BLUDAU, M. GIERER et G. ERTL. « STRUCTURAL PROPERTIES OF ALKALI-METAL ATOMS ADSORBED ON Ru(0001) ». Surface Review and Letters 02, no 03 (juin 1995) : 409–22. http://dx.doi.org/10.1142/s0218625x95000376.

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The structural properties of the ordered overlayers of Li, Na, K, Rb , and Cs on Ru (0001) are summarized. The major result is that the adsorption site depends on the coverage while the hard-sphere radii of the alkali-metal atoms do not change (if corrected for different numbers of coordination). This comparison also emphasizes the singular behavior of Cs for which adsorption takes place over single Ru atoms at a Cs coverage of 0.25. While on other close-packed substrate surfaces potassium and rubidium occupy ontop positions at low temperatures, this has not been found with Ru (0001). This finding points towards the important role of the substrate. For the ontop adsorption to be favored, an inward displacement of the substrate atoms directly underneath the alkali-metal atoms by a substantial amount is necessary which results in the formation of a quasisevenfold-coordinated bond geometry in connection with a reduction of the dipole-dipole repulsion. The stiffness of the substrate determines the energy cost for this local reconstruction, and consequently ontop adsorption on the hard Ru (0001) substrate has only been observed for the biggest alkali metal Cs where the energy difference between various adsorption sites [on the unrelaxed Ru (0001) surface] is assumed to be small. In order to force potassium to reside in the ontop position, the Ru (0001) surface has to be “softened” which task was accomplished by adding CO molecules to the K-(2×2) overlayer.
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Sturm, J. M., C. J. Lee et F. Bijkerk. « Reactions of ethanol on Ru(0001) ». Surface Science 612 (juin 2013) : 42–47. http://dx.doi.org/10.1016/j.susc.2013.02.009.

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del Campo, Valeria, Julián-David Correa, Jonathan Correa-Puerta, Daniel Kroeger et Patricio Häberle. « Unoccupied electronic states of Ru(0001) ». Surface Science 653 (novembre 2016) : 163–68. http://dx.doi.org/10.1016/j.susc.2016.07.005.

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Carabineiro, S. A. C., A. V. Matveev, V. V. Gorodetskii et B. E. Nieuwenhuys. « Selective oxidation of ammonia over Ru(0001) ». Surface Science 555, no 1-3 (avril 2004) : 83–93. http://dx.doi.org/10.1016/j.susc.2004.02.022.

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Herron, Jeffrey A., Scott Tonelli et Manos Mavrikakis. « Atomic and molecular adsorption on Ru(0001) ». Surface Science 614 (août 2013) : 64–74. http://dx.doi.org/10.1016/j.susc.2013.04.002.

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Rakocevic, Z., S. Strbac et R. J. Behm. « Interrupted-flux deposition : Ni on Ru(0001) ». Thin Solid Films 517, no 2 (novembre 2008) : 709–13. http://dx.doi.org/10.1016/j.tsf.2008.08.116.

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Nilsson, Anders. « Atom Specific Ultrafast Surface Chemistry using a Soft X-ray Laser ». Acta Crystallographica Section A Foundations and Advances 70, a1 (5 août 2014) : C124. http://dx.doi.org/10.1107/s2053273314098751.

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Catalysis is central for many chemical energy transformations that occur at interfaces. One of the dreams is to follow catalytic reactions in real time from reactants over various intermediates to products. The prospective for the study of chemical reactions on surfaces using X-ray free-electron lasers (Linac Coherent Light Source, or LCLS, at SLAC National Accelerator Laboratory) will be presented. We induced the hot electron and phonon mediated excitation of adsorbates on Ru(0001) with synchronized excitation by a femtosecond optical laser pulse. We have followed the ultrafast evolution of the bond distortions, weakening and breaking, using x-ray absorption spectroscopy and x ray emission spectroscopy resonantly tuned to the oxygen core level with ultrashort x-ray pulses delivered from LCLS. We can directly follow the time evolution of the molecular orbitals in an atom-specific way on a subpicosecond timescale. Three examples will be shown CO desorption, Oxygen activation and CO oxidation on Ru(0001).
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Tautermann, Christofer S., Bernd Wellenzohn et David C. Clary. « The thermodesorption mechanism of ammonia from Ru(0001) ». Surface Science 600, no 5 (mars 2006) : 1054–59. http://dx.doi.org/10.1016/j.susc.2005.12.032.

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Hamad, B. A. « Structural and dynamical properties of Ru(0001) surface ». Surface Science 602, no 24 (décembre 2008) : 3654–59. http://dx.doi.org/10.1016/j.susc.2008.09.020.

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Yang, Shizhong, Guang-Lin Zhao et James M. Phillips. « The electronic structures of commensurate Ru(0001)–(3×3)–4Kr and Ru(0001)–(5×5)–Kr using density functional theory ». Surface Science 604, no 11-12 (juin 2010) : 1022–28. http://dx.doi.org/10.1016/j.susc.2010.03.015.

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41

Park, C., E. Bauer et H. Poppa. « A re-examination of the Cu/Ru(0001) system ». Surface Science 187, no 1 (août 1987) : 86–97. http://dx.doi.org/10.1016/s0039-6028(87)80123-1.

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42

Schick, M., J. Schäfer, K. Kalki, G. Ceballos, P. Reinhardt, H. Hoffschulz et K. Wandelt. « Miscibility within monolayer AgCu films on Ru(0001) ». Surface Science 287-288 (mai 1993) : 960–63. http://dx.doi.org/10.1016/0039-6028(93)91108-2.

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STAMPFL, C. « DENSITY FUNCTIONAL THEORY STUDY OF Na ON Al(111) AND O ON Ru(0001) ». Surface Review and Letters 03, no 04 (août 1996) : 1567–77. http://dx.doi.org/10.1142/s0218625x96002564.

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The success of density functional theory for the description of the adsorption of atoms on surfaces is well established and, based on recent calculations using gradient corrections, it has been shown that it also describes well the dissociative adsorption of molecules at surfaces — admittedly, however, the database for reactions at surfaces is still somewhat small. In this paper the power of density functional theory calculations is demonstrated through investigations for two different adsorption systems, namely one with a strongly electropositive adsorbate [Na on Al(111)] and one with a strongly electronegative adsorbate [O on Ru(0001)]. In each case, new hitherto unexpected adsorbate phases have been predicted by the theory: for Na on Al(111) the stability of a “four-layer” surface alloy was identified while for O on Ru(0001) it was predicted that the formation of a (1×1)-O adlayer should be possible which implies that the apparent saturation coverage of Θo=1/2 is due to kinetic hindering.
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Lei, T., M. S. Zei et G. Ertl. « Electrocatalytic oxidation of CO on Pt-modified Ru(0001) electrodes ». Surface Science 581, no 2-3 (mai 2005) : 142–54. http://dx.doi.org/10.1016/j.susc.2005.02.037.

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Jakob, P., et A. Schlapka. « CO adsorption on epitaxially grown Pt layers on Ru(0001) ». Surface Science 601, no 17 (septembre 2007) : 3556–68. http://dx.doi.org/10.1016/j.susc.2007.06.035.

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Greenlief, C. M., P. L. Radloff, X. L. Zhou et J. M. White. « The formation and decomposition kinetics of ethylidyne on Ru(0001) ». Surface Science 191, no 1-2 (janvier 1987) : 93–107. http://dx.doi.org/10.1016/s0039-6028(87)81050-6.

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Ulstrup, Søren, Paolo Lacovig, Fabrizio Orlando, Daniel Lizzit, Luca Bignardi, Matteo Dalmiglio, Marco Bianchi et al. « Photoemission investigation of oxygen intercalated epitaxial graphene on Ru(0001) ». Surface Science 678 (décembre 2018) : 57–64. http://dx.doi.org/10.1016/j.susc.2018.03.017.

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Li, Tianbai, et Jory A. Yarmoff. « The orientation of CO intercalated between graphene and Ru(0001) ». Surface Science 680 (février 2019) : 6–10. http://dx.doi.org/10.1016/j.susc.2018.10.009.

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Hager, T., H. Rauscher et R. J. Behm. « Interaction of CO with PdCu surface alloys supported on Ru(0001) ». Surface Science 558, no 1-3 (juin 2004) : 181–94. http://dx.doi.org/10.1016/j.susc.2004.04.001.

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Männig, A., Z. Zhao, D. Rosenthal, K. Christmann, H. Hoster, H. Rauscher et R. J. Behm. « Structure and growth of ultrathin titanium oxide films on Ru(0001) ». Surface Science 576, no 1-3 (février 2005) : 29–44. http://dx.doi.org/10.1016/j.susc.2004.11.039.

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