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Current Sample Preparation and Analytical Capabilities of the Radiocarbon Laboratory at CologneAMS

Published online by Cambridge University Press:  26 April 2019

J Rethemeyer*
Affiliation:
Institute of Geology and Mineralogy, University of Cologne, Cologne, Germany
M Gierga
Affiliation:
Institute of Geology and Mineralogy, University of Cologne, Cologne, Germany
S Heinze
Affiliation:
Institute of Nuclear Physics, University of Cologne, Cologne, Germany
A Stolz
Affiliation:
Institute of Nuclear Physics, University of Cologne, Cologne, Germany
A Wotte
Affiliation:
Institute of Geology and Mineralogy, University of Cologne, Cologne, Germany
P Wischhöfer
Affiliation:
Institute of Geology and Mineralogy, University of Cologne, Cologne, Germany
S Berg
Affiliation:
Institute of Geology and Mineralogy, University of Cologne, Cologne, Germany
JO Melchert
Affiliation:
Institute of Geology and Mineralogy, University of Cologne, Cologne, Germany
A Dewald
Affiliation:
Institute of Nuclear Physics, University of Cologne, Cologne, Germany
*
*Corresponding author. Email: janet.rethemeyer@uni-koeln.de.
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Abstract

This work summarizes the methodical capabilities, improvements, and new developments in the radiocarbon laboratory of the accelerator mass spectrometry (AMS) facility at the University of Cologne, Germany, which was established in 2010. During the past years, the laboratory has specialized in the analysis of small and gaseous samples. We thus, recently installed a second ion source dedicated for radiocarbon (14C) analysis of CO2 samples at our 6 MV Tandetron AMS from High Voltage Engineering Europe B.V. that is coupled with the gas injection system from Ionplus and an EuroVector EA 3000 elemental analyzer. This work summarizes all pretreatment methods and analytical facilities established in our laboratory during the last years including 14C analysis of individual organic compounds and of CO2 trapped on molecular sieves. We also report different blank values including our long-term blank since 2011, which is for normal-sized, solid samples (650–1000 µg C) 0.0012 ± 0.0004 F14C (54,305 ± 2581 yr BP, n = 484). The precision obtained for modern samples measured as graphite is 0.5% and for gaseous samples injected with the GIS ≤2%.

Information

Type
Conference Paper
Copyright
© 2019 by the Arizona Board of Regents on behalf of the University of Arizona 
Figure 0

Table 1 Total number of samples per sample type prepared since 2011 in our laboratory.

Figure 1

Figure 1 Blank values (black circles) and 12C beam current (open circles) versus Fe:C ratio generated with 14C-free coal (POC#3; 1 mg C) graphitized with various amounts of Fe as catalyst (3–12 mg Fe).

Figure 2

Figure 2 (A) Blank levels (in F14C) based on measurements of normal-sized 14C-free coal (POC#3, 650–1000 µg C) graphitized and analyzed since 2011. Results shown are not blank corrected. (B) Results for normal-sized oxalic acid (OX-II) standards (650–1000 µg C) measured since the installation of the laboratory in 2011 are given with blank subtraction.

Figure 3

Figure 3 14C concentrations of blank material (coal, POC#3) versus sample size using different tin vessels for EA combustion (circles: tin boats 4 × 4 × 11 mm; squares: tin boats 8 × 8 × 15 mm; triangles: tin capsules 0.05 mL). The curves are based on the model of contamination corresponding to 0.92 µg C modern contamination (usual tin boats and capsules, black line) and 1.42 µg C modern contamination (larger tin boats).

Figure 4

Figure 4 14C contents of a modern (a) and fossil (b) standard isolated with pc-GC versus sample size with 2-sigma uncertainty. The solid line represents the 14C content of the unprocessed standard.

Figure 5

Table 2 Results for reference materials from the SIRI inter-comparison.