2016
DOI: 10.1016/j.susc.2015.11.005
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Ethylene hydrogenation catalysis on Pt(111) single-crystal surfaces studied by using mass spectrometry and in situ infrared absorption spectroscopy

Abstract: The catalytic hydrogenation of ethylene promoted by a Pt(111) single crystal was studied by using a ultrahigh-vacuum surface-science instrument equipped with a so-called high-pressure cell. Kinetic data were acquired continuously during the catalytic conversion of atmosphericpressure mixtures of ethylene and hydrogen by using mass spectrometry while simultaneously characterizing the surface species in operando mode by reflection-absorption infrared spectroscopy (RAIRS). Many observations reported in previous s… Show more

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Cited by 25 publications
(21 citation statements)
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“…A long-travel manipulator is used to transfer the sample between this main analytical tier of the UHV chamber and a second level set up to carry out RAIRS experiments. The arrangement used for this technique is similar to that of another instrument available in our laboratory for catalytic studies. ,, The IR beam from a Bruker Tensor 27 Fourier-transform infrared (FTIR) spectrometer is directed through a polarizer and a NaCl window into the UHV environment and focused at grazing incidence (∼85° from the surface normal) onto the sample by using a spherical mirror (ϕ = 3 in., f = 6 in.). The reflected beam is then collected by a second spherical mirror (after going through a second NaCl window) and focused onto a narrow-band mercury–cadmium–telluride (MCT) detector.…”
Section: Methodsmentioning
confidence: 99%
“…A long-travel manipulator is used to transfer the sample between this main analytical tier of the UHV chamber and a second level set up to carry out RAIRS experiments. The arrangement used for this technique is similar to that of another instrument available in our laboratory for catalytic studies. ,, The IR beam from a Bruker Tensor 27 Fourier-transform infrared (FTIR) spectrometer is directed through a polarizer and a NaCl window into the UHV environment and focused at grazing incidence (∼85° from the surface normal) onto the sample by using a spherical mirror (ϕ = 3 in., f = 6 in.). The reflected beam is then collected by a second spherical mirror (after going through a second NaCl window) and focused onto a narrow-band mercury–cadmium–telluride (MCT) detector.…”
Section: Methodsmentioning
confidence: 99%
“…The experiments reported here were all carried out in a UHV chamber equipped with several techniques for the cleaning and characterization of the surface as well as with a catalytic reactor where kinetic measurements can be carried out. The details of this instrumentation and the procedures used for the experiments are discussed in detail in previous publications. , Briefly, a platinum single crystal cut in the (111) orientation was mounted on a manipulator used for sample transfer between the two stages of the instrument and for surface alignment, and also for controlled cooling or heating to any temperature between approximately 100 and 1100 K (as measured using a chromel–alumel thermocouple spotwelded to the side). Most of the initial surface cleaning and preparation of this crystal was carried out before each experiment in the main UHV chamber, which is equipped with an ion gun for surface sputtering, a mass spectrometer for the analysis of the gas composition, and a set of controlled leak valves for gas dosing.…”
Section: Methodsmentioning
confidence: 99%
“…Typical data from such experiments are reported in the left panel of Figure , in this case for a D 2 :C 2 D 4 40:1 ratio and a total flux of 8000 ML/s (top, red trace). A second mass spectrum (bottom, blue trace) is reported for comparison, from a more conventional experiment carried out by using a so-called high-pressure cell, which is used to isolate the Pt surface from the UHV environment and enclose it in a small volume that can be pressurized and used as a batch reactor. , The fact that both deuteration and H–D isotope scrambling take place in both of these experiments is immediately apparent by the detection of significant signal intensities all the way to 36 amu. On the other hand, the final product distributions are clearly different in each case.…”
mentioning
confidence: 99%