TY - JOUR
T1 - On the interference of Kr during carbon isotope analysis of methane using continuous-flow combustion–isotope ratio mass spectrometry
AU - Schmitt, J.
AU - Seth, B.
AU - Bock, M
AU - van der Veen, C.
AU - Möller, L.
AU - Sapart, C.J.
AU - Prokopiou, M.
AU - Sowers, T.
AU - Röckmann, T.
AU - Fischer, H
PY - 2013
Y1 - 2013
N2 - Stable carbon isotope analysis of methane ( 13C
of CH4) on atmospheric samples is one key method to constrain
the current and past atmospheric CH4 budget. A frequently
applied measurement technique is gas chromatography
(GC) isotope ratio mass spectrometry (IRMS) coupled to
a combustion-preconcentration unit. This report shows that
the atmospheric trace gas krypton (Kr) can severely interfere
during the mass spectrometric measurement, leading to significant
biases in 13C of CH4, if krypton is not sufficiently
separated during the analysis. According to our experiments,
the krypton interference is likely composed of two individual
effects, with the lateral tailing of the doubly charged
86Kr peak affecting the neighbouring m/z 44 and partially
the m/z 45 Faraday cups. Additionally, a broad signal affecting
m/z 45 and especially m/z 46 is assumed to result from
scattered ions of singly charged krypton. The introduced bias
in the measured isotope ratios is dependent on the chromatographic
separation, the krypton-to-CH4 mixing ratio in the
sample, the focusing of the mass spectrometer as well as
the detector configuration and can amount to up to several
per mil in 13C. Apart from technical solutions to avoid this
interference, we present correction routines to a posteriori
remove the bias.
AB - Stable carbon isotope analysis of methane ( 13C
of CH4) on atmospheric samples is one key method to constrain
the current and past atmospheric CH4 budget. A frequently
applied measurement technique is gas chromatography
(GC) isotope ratio mass spectrometry (IRMS) coupled to
a combustion-preconcentration unit. This report shows that
the atmospheric trace gas krypton (Kr) can severely interfere
during the mass spectrometric measurement, leading to significant
biases in 13C of CH4, if krypton is not sufficiently
separated during the analysis. According to our experiments,
the krypton interference is likely composed of two individual
effects, with the lateral tailing of the doubly charged
86Kr peak affecting the neighbouring m/z 44 and partially
the m/z 45 Faraday cups. Additionally, a broad signal affecting
m/z 45 and especially m/z 46 is assumed to result from
scattered ions of singly charged krypton. The introduced bias
in the measured isotope ratios is dependent on the chromatographic
separation, the krypton-to-CH4 mixing ratio in the
sample, the focusing of the mass spectrometer as well as
the detector configuration and can amount to up to several
per mil in 13C. Apart from technical solutions to avoid this
interference, we present correction routines to a posteriori
remove the bias.
U2 - 10.5194/amt-6-1425-2013
DO - 10.5194/amt-6-1425-2013
M3 - Article
SN - 1867-1381
VL - 6
SP - 1425
EP - 1445
JO - Atmospheric Measurement Techniques
JF - Atmospheric Measurement Techniques
ER -