Jean-Pierre van Helden

Prof. Dr. Jean-Pierre van Helden

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Research Focus & Metrics

Academic Career Length

25Years (2002-Present)

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

Representative Publications

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13 August 2015 in Plasma Sources Science and Technology
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Journal Article
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SRStephan Reuter
Stephan Reuter
JSJoao Santos Sousa
Joao Santos Sousa
GSGabi Daniel Stancu
Gabi Daniel Stancu
JHJean-Pierre van Helden
Jean-Pierre van Helden

15 February 2007 in Journal of Applied Physics
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JHJean-Pierre van Helden
Jean-Pierre van Helden
WWW. Wagemans
W. Wagemans
GYG. Yagci
G. Yagci
RZR. A. B. Zijlmans
R. A. B. Zijlmans
DSD. C. Schram
D. C. Schram
JRJ. Röpcke
J. Röpcke
We investigated the efficiency and formation mechanism of ammonia generation in recombining plasmas generated from mixtures of N2 and H2 under various plasma conditions. In contrast to the Haber-Bosch process, in which the molecules are dissociated on a catalytic surface, under these plasma conditions the precursor molecules, N2 and H2 , are already dissociated in the gas phase. Surfaces are thus exposed to large fluxes of atomic N and H radicals. The ammonia production turns out to be strongly dependent on the fluxes of atomic N and H radicals to the surface. By optimizing the atomic N and H fluxes to the surface using an atomic nitrogen and hydrogen source ammonia can be formed efficiently, i.e., more than 10% of the total background pressure is measured to be ammonia. The results obtained show a strong similarity with results reported in literature, which were explained by the production of ammonia at the surface by stepwise addition reactions between adsorbed nitrogen and hydrogen containing radicals at the surface and incoming N and H containing radicals. Furthermore, our results indicate that the ammonia production is independent of wall material. The high fluxes of N and H radicals in our experiments result in a passivated surface, and the actual chemistry, leading to the formation of ammonia, takes place in an additional layer on top of this passivated surface.

11 December 2012 in Analytical Chemistry
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LCLuca Ciaffoni
Luca Ciaffoni
GHGus Hancock
Gus Hancock
JHJeremy J. Harrison
Jeremy J. Harrison
JHJean-Pierre van Helden
Jean-Pierre van Helden
CLCathryn E. Langley
Cathryn E. Langley
SWSimon Wood
Simon Wood

18 May 2009 in Applied Physics Letters
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GHG. Hancock
G. Hancock
JHJean-Pierre van Helden
Jean-Pierre van Helden
RPR. Peverall
R. Peverall
GRG. A. D. Ritchie
G. A. D. Ritchie
RWR. J. Walker
R. J. Walker
A continuous wave external cavity quantum cascade laser (EC-QCL) operating between 1872 and 1958 cm−1 has been used to make rotationally resolved measurements in the fundamental band of nitric oxide at 140 mTorr, and the ν2 band of water at atmospheric pressure. These measurements demonstrate the advantages of wide tunability and high resolution of the EC-QCL system. From direct absorption spectroscopy on nitric oxide a laser bandwidth of 20 MHz has been deduced and a sensitivity of 8.4×10−4 cm−1 Hz−1/2 was achieved. Wavelength modulation spectroscopy using current modulation enhances the sensitivity by a factor of 23 to 3.7×10−5 cm−1 Hz−1/2 .

12 October 2007 in The Journal of Physical Chemistry A
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JHJean-Pierre van Helden
Jean-Pierre van Helden
POP. J. van Den Oever
P. J. van Den Oever
WKW. M. M. Kessels
W. M. M. Kessels
MSM. C. M. van de Sanden
M. C. M. van de Sanden
DSD. C. Schram
D. C. Schram
RER. Engeln
R. Engeln

23 September 2013 in Applied Physics Letters
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JHJean-Pierre van Helden
Jean-Pierre van Helden
NLNorbert Lang
Norbert Lang
UMU. Macherius
U. Macherius
HZH. Zimmermann
H. Zimmermann
JRJ. Röpcke
J. Röpcke
Trace gas sensing in the mid-infrared using quantum cascade lasers (QCLs) promises high specificity and sensitivity. We report on the performance of a simple cavity enhanced absorption spectroscopy (CEAS) sensor using a continuous wave external-cavity QCL at 7.4 μm. A noise-equivalent absorption coefficient αmin of 2.6 × 10–8 cm–1 in 625 s was achieved, which corresponds to a detection limit of 6 ± 1 ppb of CH4 in 15 millibars air for the R(3) transition at 1327.074 cm–1. This is the highest value of noise-equivalent absorption and among the longest effective path length (1780 m) reported to date with QCL-based CEAS.