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Development of 14C Dating of Mortars at ETH Zurich

Published online by Cambridge University Press:  02 June 2020

Irka Hajdas*
Affiliation:
Laboratory of Ion Beam Physics, ETH Zurich, Otto-Stern-Weg 5, 8093 Zurich, Switzerland
Mantana Maurer
Affiliation:
Laboratory of Ion Beam Physics, ETH Zurich, Otto-Stern-Weg 5, 8093 Zurich, Switzerland
Maria Belen Röttig
Affiliation:
Laboratory of Ion Beam Physics, ETH Zurich, Otto-Stern-Weg 5, 8093 Zurich, Switzerland
*
*Corresponding author. Email: hajdas@phys.ethz.ch.
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Abstract

The ages of mortars and plaster can help reveal the history of monuments, their construction, or restoration times. However, these anthropogenic carbonates pose a challenge when it comes to separation of the atmospheric radiocarbon (14C) signal of the CO2 fixed in the mortar at the time of consolidation, i.e., the time of binder formation. The variety and heterogeneity of mortars require individual assessments of each sample and 14C results. Here we present our current preparation method and summarize experience based on results collected during the last 20 years of mortar dating at the ETH laboratory.

Information

Type
Research Article
Copyright
© 2020 by the Arizona Board of Regents on behalf of the University of Arizona
Figure 0

Table 1 Overview of samples analyzed by the ETH laboratory as a part of the MODIS inter-comparison (Hajdas et al. 2017). The starting mass of the samples is on the order of 30–50 mg.

Figure 1

Figure 1 Results obtained by the ETH laboratory for Sample 1 in the MODIS intercomparison (Hajdas et al. 2017). The numbers indicate fractions: 1 = 1–3 sec, 2 = 4–6 sec, 3 = 7–9 sec, and 4 = 10–12 sec dissolution time window. The fine fraction of 46–75 μm was used. The combined value of all 4 fractions is 491 ± 21 BP (χ2-test: df = 3, T = 6.0 [5% 7.8]) was calculated using the OxCal Combine model function (Ramsey 2009).

Figure 2

Figure 2 Results obtained by the ETH laboratory for Sample 2 in the MODIS intercomparison (Hajdas et al. 2017). The numbers indicate fractions: 1 = 1–3 sec, 2 = 4–6 sec, 3 = 7–9 sec, and 4 = 10–12 sec dissolution time window. The fine fraction distributed in MODIS exercise was grain size <500 μm but fraction 45–63 μm was used for dating. The first fraction had very low carbon content resulting in high uncertainty. The combined value for the first and second fractions is 2352 ± 69 BP.

Figure 3

Figure 3 Results obtained by the ETH laboratory for Sample 3 in the MODIS intercomparison (Hajdas et al. 2017). The numbers indicate fractions: 1 = 1–3 sec, 2 = 4–6 sec, 3 = 7–9 sec, and 4 = 10–12 sec dissolution time window. Two preparations were performed: one on a fraction 45–63 μm (circles) and one on fraction <45 μm (triangles). In addition, the charcoal sample found in the mortar was dated at 1313 ± 22 BP. Note the significant change of radiocarbon ages with the increasing fraction number (dissolution time).

Figure 4

Figure 4 Results obtained by the ETH laboratory for Sample 4 in the MODIS intercomparison (Hajdas et al. 2017). The numbers indicate fractions: 1 = 1–3 sec, 2 = 4–6 sec, 3 = 7–9 sec, and 4 = 10–12 sec dissolution time window. Two preparations were performed on fraction 32–63 μm (circle) and on a fraction smaller than 32 μm (triangles). Note that the three first fractions of both preparations agree in the 2-σ range.