Solid catalysts with ionic liquid layers (SCILLs) have recently attracted a lot of attention, as the ionic liquid (IL) coating can give rise to drastically improved selectivity. Here, we studied the interaction of the IL 1-butyl-1-methylpyrrolidinium bis(trifluoromethylsulfonyl)-imide [C 4 C 1 Pyr]-[NTf 2 ] with Pt(111) and Pt nanoparticles (NPs) on highly oriented pyrolytic graphite under ultrahigh vacuum conditions. The IL film on Pt(111) and on the Pt NPs consists of a strongly bound monolayer and a weakly bound bulk phase. In the monolayer, [NTf 2 ] − adopts cis conformation and binds via the SO 2 groups. Adsorption of [NTf 2 ] − at Pt defect sites is preferred to adsorption at terraces, whereas preadsorbed CO blocks the adsorption at defects. Further, IL coadsorption leads to desorption and displacement of on-top CO on terraces, whereas CO resides in the bridging position. IL multilayers desorb at 380 K, whereas the strongly adsorbed monolayer on Pt resides and gradually desorbs and decomposes between 400 and 500 K. Finally, we studied the permeability of IL layers for CO by pressure modulation experiments in combination with in situ infrared reflection absorption spectroscopy. We show that the IL multilayer completely blocks CO adsorption, whereas CO easily penetrates the IL monolayer film and forms a mixed adsorbate phase. It is noteworthy that dynamic CO adsorption is much more facile on Pt NPs than on Pt(111). Our results suggest that strongly adsorbed IL monolayers may play an important role in real SCILLs.
Fuel
cells can be operated directly by oxidation of isopropyl alcohol
(IPA) to acetone (ACE). If the product ACE is hydrogenated, IPA is
formed again. In this way, IPA serves as a rechargeable electrofuel.
In this work, we study the oxidation of IPA at Pt electrodes using
several complementary experimental methods, including cyclic voltammetry
(CV), electrochemical real-time mass spectrometry (EC-RTMS), and electrochemical
infrared reflection absorption spectroscopy (EC-IRRAS), in combination
with density functional theory (DFT) to assign the vibrational modes
of IPA and ACE. Different types of Pt electrodes are investigated,
namely single crystalline Pt(111) surfaces, polycrystalline Pt, and
nanostructured tubular Pt electrodes. The onset of the IPA oxidation
on the Pt electrodes is observed at 0.3 VRHE, yielding
ACE with high selectivity. At potentials above 0.9 VRHE, the formation of Pt oxide inhibits the reaction. The only side
reaction observed is the formation of small amounts of CO2. We show that adsorbed ACE is formed at the Pt electrodes poisoning
the surface. On nanotubular electrodes with high surface area, ACE
stays mainly adsorbed on the surface, and only a small fraction desorbs.
These observations suggest that poisoning of the Pt electrode by adsorbed
ACE limits the oxidation of IPA.
We have investigated the surface chemistry of the polycyclic valence-isomer pair norbornadiene (NBD) and quadricyclane (QC) on Pt(111). The NBD/QC system is considered to be a prototype for energy storage in strained organic compounds. By using a multimethod approach, including UV photoelectron, high-resolution X-ray photoelectron, and IR reflection-absorption spectroscopic analysis and DFT calculations, we could unambiguously identify and differentiate between the two molecules in the multilayer phase, which implies that the energy-loaded QC molecule is stable in this state. Upon adsorption in the (sub)monolayer regime, the different spectroscopies yielded identical spectra for NBD and QC at 125 and 160 K, when multilayer desorption takes place. This behavior is explained by a rapid cycloreversion of QC to NBD upon contact with the Pt surface. The NBD adsorbs in a η :η geometry with an agostic Pt-H interaction of the bridgehead CH subunit and the surface. Strong spectral changes are observed between 190 and 220 K because the hydrogen atom that forms the agostic bond is broke. This reaction yields a norbornadienyl intermediate species that is stable up to approximately 380 K. At higher temperatures, the molecule dehydrogenates and decomposes into smaller carbonaceous fragments.
Dwindling fossil fuels force humanity to search for new energy production routes. Besides energy generation, its storage is a crucial aspect. One promising approach is to store energy from the sun chemically in strained organic molecules, so-called molecular solar thermal (MOST) systems, which can release the stored energy catalytically. A prototypical MOST system is norbornadiene/quadricyclane (NBD/QC) whose energy release and surface chemistry need to be understood. Besides important key parameters such as molecular weight, endergonic reaction profiles, and sufficient quantum yields, the position of the absorption onset of NBD is crucial to cover preferably a large range of sunlight’s spectrum. For this purpose, one typically derivatizes NBD with electron-donating and/or electron-accepting substituents. To keep the model system simple enough to be investigated with photoemission techniques, we introduced bromine atoms at the 2,3-position of both compounds. We study the adsorption behavior, energy release, and surface chemistry on Ni(111) using high-resolution X-ray photoelectron spectroscopy (HR-XPS), UV photoelectron spectroscopy, and density functional theory calculations. Both Br2-NBD and Br2-QC partially dissociate on the surface at ∼120 K, with Br2-QC being more stable. Several stable adsorption geometries for intact and dissociated species were calculated, and the most stable structures are determined for both molecules. By temperature-programmed HR-XPS, we were able to observe the conversion of Br2-QC to Br2-NBD in situ at 170 K. The decomposition of Br2-NBD starts at 190 K when C–Br bond cleavage occurs and benzene and methylidene are formed. For Br2-QC, the cleavage already occurs at 130 K when cycloreversion to Br2-NBD sets in.
Solid catalysts with ionic liquid
layers (SCILLs) show improved
performance as compared to ionic liquid (IL)-free catalysts. To realize
the beneficial IL-induced modification, the IL layer should be stable
under reaction conditions but also permeable for gaseous reactants
entering through the IL phase. Herein, we applied (polarization modulation-)
infrared reflection absorption spectroscopy ((PM-)IRAS) to investigate
the CO permeability of model SCILL systems. We investigated three
different IL model systems prepared by physical vapor deposition (PVD)
in ultrahigh vacuum (UHV) on atomically clean Pt(111), namely, 1-butyl-1-methylpyrrolidinium bis(trifluoromethylsulfonyl)imide ([C4C1Pyr][NTf2]), 1-ethyl-3-methylimidazolium bis(trifluoromethylsulfonyl)imide ([C2C1Im][NTf2]), and 1-butyl-1-methylpyrrolidinium trifluoromethanesulfonate
([C4C1Pyr][OTf]). The adsorption geometries
of the anions depend on the surface structure, IL coverage, and precoverage
of CO. At room temperature, IL multilayers of randomly oriented species
grow on top of strongly adsorbed wetting layers. Upon heating, a partial
wetting transition induces the coexistence of an IL wetting monolayer
film with three-dimensional droplets. Gas-phase CO does not permeate
through IL multilayers, while it penetrates the IL wetting monolayer
leading to mixed IL/CO films. The partial dewetting transition and
the permeability differ drastically with the temperature and IL. Consequently,
the morphology of the IL films could be a factor that determines the
catalytic behavior of SCILLs to a significant extent.
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