Mass spectrometry is the technique of separating and counting the constituent atoms of a sample according to their mass. Accelerator Mass Spectrometry (AMS) requires that a charged particle accelerator be added to the equipment conventionally used in mass spectrometry, increasing the sensitivity of the system for detecting rare atoms or isotopes.

The most common type of sample analysed by AMS is radiocarbon or 14C. The following paragraphs use the analysis of 14C as an example to introduce the concepts involved in AMS.

A New Approach to Carbon Dating

In 1977, a major breakthrough took place in the technique of radiocarbon dating. It was discovered that individual carbon-14 atoms from a natural sample could be counted directly, a process which takes considerably less time and sample material than the conventional method of counting the infrequent carbon-14 beta-decays. The equipment used to make this discovery was similar to that used in mass spectrometry but with the addition of higher voltage acceleration and charged particle counting apparatus used by nuclear structure physicists.

The Advantages of Higher Energy

The carbon-14 isotope is such a small fraction of modern carbon (1.2 x 10-12) that it lies well below the detection limit for conventional mass spectrometry. This limit is set by the presence of interfering atomic and molecular species of the same mass as 14C, e.g. 14N, 12CH2 and 13CH. 14N, the only atomic interference, can be eliminated by choosing negative ions to analyse, because these are unstable and do not live long enough to enter the accelerator. The molecular interferences are eliminated by removing a sufficient number of electrons to break apart the molecules, a process which requires acceleration of the ions to higher energies than in conventional mass spectrometry. The increased energy acquired by the ions has the additional advantage that the high velocity 14C ions can be individually identified and distinguished from other background ions.

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