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Selective hydrogenation of 2-methylnaphthalene by heterostructured Ni-NiO-based catalysts for 6-methyl-1,2,3,4-tetrahydronaphthalene. MOLECULAR CATALYSIS 2022. [DOI: 10.1016/j.mcat.2022.112537] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 11/18/2022]
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Werkovits A, Jeindl A, Hörmann L, Cartus JJ, Hofmann OT. Toward Targeted Kinetic Trapping of Organic–Inorganic Interfaces: A Computational Case Study. ACS PHYSICAL CHEMISTRY AU 2022; 2:38-46. [PMID: 35098244 PMCID: PMC8796281 DOI: 10.1021/acsphyschemau.1c00015] [Citation(s) in RCA: 2] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 07/12/2021] [Revised: 09/21/2021] [Accepted: 09/23/2021] [Indexed: 11/29/2022]
Abstract
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Properties of inorganic–organic interfaces, such as their
interface dipole, strongly depend on the structural arrangements of
the organic molecules. A prime example is tetracyanoethylene (TCNE)
on Cu(111), which shows two different phases with significantly different
work functions. However, the thermodynamically preferred phase is
not always the one that is best suited for a given application. Rather,
it may be desirable to selectively grow a kinetically trapped structure.
In this work, we employ density functional theory and transition state
theory to discuss under which conditions such a kinetic trapping might
be possible for the model system of TCNE on Cu. Specifically, we want
to trap the molecules in the first layer in a flat-lying orientation.
This requires temperatures that are sufficiently low to suppress the
reorientation of the molecules, which is thermodynamically more favorable
for high dosages, but still high enough to enable ordered growth through
diffusion of molecules. On the basis of the temperature-dependent
diffusion and reorientation rates, we propose a temperature range
at which the reorientation can be successfully suppressed.
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Affiliation(s)
- Anna Werkovits
- Institute of Solid State Physics, TU Graz, NAWI Graz, Petersgasse 16/II, 8010 Graz, Austria
| | - Andreas Jeindl
- Institute of Solid State Physics, TU Graz, NAWI Graz, Petersgasse 16/II, 8010 Graz, Austria
| | - Lukas Hörmann
- Institute of Solid State Physics, TU Graz, NAWI Graz, Petersgasse 16/II, 8010 Graz, Austria
| | - Johannes J. Cartus
- Institute of Solid State Physics, TU Graz, NAWI Graz, Petersgasse 16/II, 8010 Graz, Austria
| | - Oliver T. Hofmann
- Institute of Solid State Physics, TU Graz, NAWI Graz, Petersgasse 16/II, 8010 Graz, Austria
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Marks K, Yazdi MG, Piskorz W, Simonov K, Stefanuik R, Sostina D, Guarnaccio A, Ovsyannikov R, Giangrisostomi E, Sassa Y, Bachellier N, Muntwiler M, Johansson FOL, Lindblad A, Hansson T, Kotarba A, Engvall K, Göthelid M, Harding DJ, Öström H. Investigation of the surface species during temperature dependent dehydrogenation of naphthalene on Ni(111). J Chem Phys 2019; 150:244704. [PMID: 31255092 DOI: 10.1063/1.5098533] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/15/2022] Open
Abstract
The temperature dependent dehydrogenation of naphthalene on Ni(111) has been investigated using vibrational sum-frequency generation spectroscopy, X-ray photoelectron spectroscopy, scanning tunneling microscopy, and density functional theory with the aim of discerning the reaction mechanism and the intermediates on the surface. At 110 K, multiple layers of naphthalene adsorb on Ni(111); the first layer is a flat lying chemisorbed monolayer, whereas the next layer(s) consist of physisorbed naphthalene. The aromaticity of the carbon rings in the first layer is reduced due to bonding to the surface Ni-atoms. Heating at 200 K causes desorption of the multilayers. At 360 K, the chemisorbed naphthalene monolayer starts dehydrogenating and the geometry of the molecules changes as the dehydrogenated carbon atoms coordinate to the nickel surface; thus, the molecule tilts with respect to the surface, recovering some of its original aromaticity. This effect peaks at 400 K and coincides with hydrogen desorption. Increasing the temperature leads to further dehydrogenation and production of H2 gas, as well as the formation of carbidic and graphitic surface carbon.
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Affiliation(s)
- Kess Marks
- Department of Physics, Fysikum, Stockholm University, 106 91 Stockholm, Sweden
| | - Milad Ghadami Yazdi
- SCI, Material and Nanophysics, KTH Royal Institute of Technology, 16440 Kista, Sweden
| | - Witold Piskorz
- Faculty of Chemistry, Jagiellonian University in Kraków, Gronostajowa 2, 31-387 Kraków, Poland
| | - Konstantin Simonov
- Department of Physics and Astronomy, Uppsala University, 751 20 Uppsala, Sweden
| | - Robert Stefanuik
- Department of Physics and Astronomy, Uppsala University, 751 20 Uppsala, Sweden
| | - Daria Sostina
- Paul Scherrer Institut, 5232 Villigen PSI, Switzerland
| | - Ambra Guarnaccio
- CNR-ISM-Institute of Structure of Matter-Tito Scalo Unit, C/da S. Loja, 85050 Tito Scalo, Potenza, Italy
| | - Ruslan Ovsyannikov
- Institute for Methods and Instrumentation in Synchrotron Radiation Research FG-ISRR, Helmholtz-Zentrum Berlin für Materialien und Energie, 12489 Berlin, Germany
| | - Erika Giangrisostomi
- Institute for Methods and Instrumentation in Synchrotron Radiation Research FG-ISRR, Helmholtz-Zentrum Berlin für Materialien und Energie, 12489 Berlin, Germany
| | - Yasmine Sassa
- Department of Physics, Chalmers University of Technology, SE-412 96 Göteborg, Sweden
| | | | | | | | - Andreas Lindblad
- Department of Physics and Astronomy, Uppsala University, 751 20 Uppsala, Sweden
| | - Tony Hansson
- Department of Physics, Fysikum, Stockholm University, 106 91 Stockholm, Sweden
| | - Andrzej Kotarba
- Faculty of Chemistry, Jagiellonian University in Kraków, Gronostajowa 2, 31-387 Kraków, Poland
| | - Klas Engvall
- Department of Chemical Engineering, KTH Royal Institute of Technology, 100 44 Stockholm, Sweden
| | - Mats Göthelid
- SCI, Material and Nanophysics, KTH Royal Institute of Technology, 16440 Kista, Sweden
| | - Dan J Harding
- Department of Chemical Engineering, KTH Royal Institute of Technology, 100 44 Stockholm, Sweden
| | - Henrik Öström
- Department of Physics, Fysikum, Stockholm University, 106 91 Stockholm, Sweden
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