2017
DOI: 10.1007/s00340-017-6681-3
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A convenient setup for laser-induced fluorescence imaging of both CO and CO2 during catalytic CO oxidation

Abstract: [2]. The reaction process is well known under ultra-high vacuum (UHV) conditions where gas flows and gas distribution around a sample are often neglected. However, the number of molecules interacting with the catalyst surface increases significantly at elevated pressures, and as a result, a change in the gas composition close to the surface may lead to a change of the surface structure [3,4]. Therefore, it is essential to obtain in-situ knowledge of the gas composition close to an operating catalyst to achieve… Show more

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Cited by 23 publications
(18 citation statements)
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“…More details regarding the gas system, optical access capabilities, and possible geometries of the high-pressure part are presented in Ref. 30.…”
Section: Methodsmentioning
confidence: 99%
“…More details regarding the gas system, optical access capabilities, and possible geometries of the high-pressure part are presented in Ref. 30.…”
Section: Methodsmentioning
confidence: 99%
“…We have used PLIF to visualize the concentration or the distribution of gas phase CO and CO 2 above two different Pd single crystals. Two different laser systems and reactors were used for probing CO and CO 2 , but the layout of the experimental setup was the same in both experiments .…”
Section: Experimental Methodsmentioning
confidence: 99%
“…Our contribution in this rapid development has been in the development of High-Energy Surface X-ray Diffraction at ultrahigh X-ray energies (HESXRD) and of Planar Laser-Induced Fluorescence (PLIF) applied to catalysis, providing new experimental approaches for in situ measurements.…”
Section: Introductionmentioning
confidence: 99%
“…The experimental setup and detection scheme for the CO 2 PLIF have been described in detail previously. , The detection of CO 2 was realized by exciting the (00°0) → (10°1) combination band at ∼2.7 μm and collecting the fluorescence from the fundamental band at ∼4.3 μm. The fundamental 1064 nm laser beam with ∼350 mJ/pulse from an injection seeded single-mode Nd:YAG laser was used to pump a broad-band infrared optical parametric oscillator (IR OPO; GWU, versaScan-L 1064), generating a signal beam at ∼1.7 μm and an idler beam at ∼2.7 μm, with ∼8 and ∼7 mJ/pulse, respectively, both operating at 10 Hz.…”
Section: Methodsmentioning
confidence: 99%