Jan W. Àugustynski

Prof. Dr. Jan W. Àugustynski

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Research Focus & Metrics

Academic Career Length

32Years (1995-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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10 September 2010 in Angewandte Chemie International Edition
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RSRenata Solarska
Renata Solarska
AKAgata Królikowska
Agata Królikowska
JÀJan W. Àugustynski
Jan W. Àugustynski

30 January 2012 in Nanoscale
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RSRenata Solarska
Renata Solarska
RJRafał Jurczakowski
Rafał Jurczakowski
JÀJan W. Àugustynski
Jan W. Àugustynski
Nanostructuring of semiconductor films offers the potential means for producing photoelectrodes with improved minority charge carrier collection. Crucial to the effective operation of the photoelectrode is also the choice of a suitable electrolyte. The behaviour of the nanostructured WO3 photoanodes in methane sulfonic acid solutions, which allow one to obtain large, perfectly stable visible-light driven water splitting photocurrents, is discussed. The important effect of the electrolyte concentration upon the current distribution and the related photocurrent losses within the nanoporous photoelectrodes is pointed out.

9 December 2019 in Advanced Energy Materials
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MJMichal Jadwiszczak
Michal Jadwiszczak
KJKatarzyna Jakubow-Piotrowska
Katarzyna Jakubow-Piotrowska
PKPiotr Kedzierzawski
Piotr Kedzierzawski
KBKrzysztof Bienkowski
Krzysztof Bienkowski
JÀJan W. Àugustynski
Jan W. Àugustynski

19 May 2016 in Advanced Energy Materials
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MSMarta Sarnowska
Marta Sarnowska
KBKrzysztof Bienkowski
Krzysztof Bienkowski
PBPiotr J. Barczuk
Piotr J. Barczuk
RSRenata Solarska
Renata Solarska
JÀJan W. Àugustynski
Jan W. Àugustynski

13 October 2022 in Communications Chemistry
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KJKatarzyna Jakubow-Piotrowska
Katarzyna Jakubow-Piotrowska
BWBartlomiej Witkowski
Bartlomiej Witkowski
JÀJan W. Àugustynski
Jan W. Àugustynski
Coupling the photo-oxidation of biomass derived substrates with water splitting in a photoelectrochemical (PEC) cell is a broadly discussed approach intended to enhance efficiency of hydrogen generation at the cathode. Here, we report a PEC device employing a nanostructured semitransparent WO3 photoanode that, irradiated with simulated solar light achieves large photocurrents of 6.5 mA cm−2 through oxidation of glucose, a common carbohydrate available in nature that can be obtained by processing waste biomass. The attained photocurrents are in a large part due to the occurrence of the photocurrent doubling, where oxidation of glucose by the photogenerated positive hole is followed by injection by the formed intermediate of an electron into the conduction band of WO3. Selection of an appropriate supporting electrolyte enabled effective reforming of glucose into valuable products: gluconic and glucaric acids, erythrose and arabinose with up to 64% total Faradaic yield attained at ca 15% glucose conversion.

1 May 1995 in Journal of Applied Physics
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RKR. Kostecki
R. Kostecki
JÀJan W. Àugustynski
Jan W. Àugustynski
The use of an aqueous electrolyte containing dissolved CO2 enabled revealing of an unusually intense photoemission from a bulk silver electrode. The observed cathodic photocurrent exhibits a sharp peak at ∼360 nm corresponding to the energy of surface plasmons in silver. The amount and the spectral distribution of the photocurrent are strongly affected by the extent of roughness of the silver surface. In particular, an electrochemical roughening procedure, analogous to that leading to the surface enhancement of Raman scattering (SERS) at silver, causes appearance of a long tail on the low‐energy side of the photoemission spectra. In consequence, significant photocurrents, corresponding to a quantum yield of ∼7×10−3, are observed for the deliberately roughened silver electrodes illuminated with the wavelength of 514 nm, most frequently used in SERS experiments. It is postulated that this intense photoemission, discovered in the presence of CO2 in the solution, equally takes place in the absence of scavengers. However, in the latter case no significant photocurrents can be detected as most of the photoemitted electrons (solvated or not) return back to the electrode.