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Title:SI-TRACEABLE SCALE FOR MEASUREMENTS OF RADIOCARBON CONCENTRATION
Author(s):Hodges, Joseph T.
Contributor(s):Long, David A.; Liu, Qingnan; Fleisher, Adam J.
Subject(s):Spectroscopy as an analytical tool
Abstract:
Radiocarbon ($^{14}$C) dating of organic materials is based on measuring the $^{14}$C/$^{12}$C atomic fraction relative to the nascent value that existed when the material was formed by photosynthetic conversion of carbon dioxide present in the atmosphere. This field of measurement has numerous applications including source apportionment of anthropogenic and biogenic fuels and combustion emissions, carbon cycle dynamics, archaeology, and forensics. _x000d_ _x000d_ Accelerator mass spectrometry (AMS) is the most widely used method for radiocarbon detection because it can measure extremely small amounts of radiocarbon (background of nominally 1.2 parts-per-trillion) with high relative precision (0.4 $\%$). AMS measurements of radiocarbon are typically calibrated by reference to standard oxalic-acid (C$_2$H$_2$O$_4$) samples of known radiocativity that are derived from plant matter. Specifically, the internationally accepted absolute dating reference for so-called "modern-equivalent" radiocarbon is 95 $\%$ of the specific radioactivity in AD 1950 of the National Bureau of Standards (NBS) oxalic acid standard reference material and normalized to $\delta^{13}$C$_{VPDB}$ = 19 per mil $\footnote{M. Stuiver and H. A. Polach, \textit{Radiocarbon} \textbf{19}, (1977) 355}$. With this definition, a "modern-equivalent" corresponds to 1.176(70) parts-per-trillion of $^{14}$C relative to total carbon content._x000d_ _x000d_ As an alternative radiocarbon scale, we propose an SI-traceable method to determine $^{14}$C absolute concentration which is based on linear Beer-Lambert-law absorption measurements of selected $^{14}$C$^{16}$O$_2$ $\nu_3$-band line areas. This approach is attractive because line intensities of chosen radiocarbon dioxide transitions can be determined by $\textit{ab initio}$ calculations with relative uncertainties below 0.5 $\%$. This assumption is justified by the excellent agreement between theoretical values of line intensities and measurements for stable isotopologues of CO$_2$ $\footnote{O. L. Polyansky et al., \textit{Phys. Rev. Lett.} \textbf{114}, (2015) 243001}$. In the case of cavity ring-down spectroscopy (CRDS) measurements of $^{14}$C$^{16}$O$_2$ peak areas, we show that absolute, SI-traceable concentrations of radiocarbon can be determined through measurements of time, frequency, pressure and temperature. Notably, this approach will not require knowledge of the radiocarbon half-life and is expected to provide a stable scale that does not require an artifact standard.
Issue Date:6/21/2017
Publisher:International Symposium on Molecular Spectroscopy
Citation Info:APS
Genre:CONFERENCE PAPER/PRESENTATION
Type:Text
Language:English
URI:http://hdl.handle.net/2142/96791
DOI:10.15278/isms.2017.WE04
Date Available in IDEALS:2017-07-27


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