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PIGE - Proton Induced Gamma-ray Emission
In low energy encounters between ions and atoms, the Coulomb repulsion between the
charged ion and the nucleus of the atom prevent any close interaction between the
ion and the nucleus. However, MeV energy protons can penetrate the Coulomb barrier
on light elements and induce various nuclear reactions. Many of these reaction channels
involve the emission of gamma-rays.
Detection of nuclear reaction induced gamma-rays, and detailed characterization
of reaction cross-sections, has enabled quantitative analysis methods to
be developed. The lower Coulomb barrier of light elements makes PIGE particularly
suitable for the analysis of light elements such as Li, Be, B, F, Na, and Al.
A weakness of PIXE is the general inaccessibility of light elements (Z<13).
While complimentary tools, such as the EMP help to fill this gap for major elements, providing
routine major element data down to at least Na, the lightest elements (e.g.
H, Li, B) require nuclear reaction or recoil methods.
The Laboratoire Pierre Sue, Saclay, and the Bruyeres le Chatel nuclear
microprobe facility, Paris, have developed nuclear reaction methods
for the measurement of 1,2H, 6,7Li, 10,11B,
12C, 14N, 16O, 19F, 23Na,
24,25Mg, 27Al, 28Si, 32S
and 35Cl in minerals (Courel et al., 1991; see review by
Ryan and Griffin, 1993, and references therein). The isotopes 7Li,
19F, 23Na, 24,25Mg, 27Al,
28Si and 35Cl are determined using (p,p'gamma)
reactions (PIGE) at proton energies from less than 2 MeV up to 3.5 MeV,
suitable for simultaneous PIXE analysis of heavier elements. A similar
approach is taken by the Queen's University group (MacArthur and Ma,
1991). H is determined by elastic recoil detection (ERDA). The remaining
isotopes are determined using (d,a), (d,p), (p,a) and (p,a gamma) reactions.
The corresponding elemental detection limits for all elements between
H and F are 10-50 ppm. For the elements Na and heavier the detection
limits grow from ~200 to ~2000 ppm.
The notation used for nuclear reactions, (x,yz), denotes the incident
beam particle "x" and the reaction products "y" and "z", where "p" is a proton,
"d" is a deuteron (2H), "a" is an alpha particle (4He) and
"g" or "gamma" denotes a gamma-ray. "p'" denotes an inelastically scattered
proton; it leaves the target nucleus in an excited state.
Further Reading:
- C.G. Ryan, "The Nuclear Microprobe as a probe of earth structure and geological
processes", Nucl. Instr. Meth. B104 (1995) 377-394.
- M.B.H. Breese, D.N. Jamieson and P.J.C. King, "Materials
Analysis using a Nuclear Microprobe", Wiley and Sons, New York,
1996.
References:
- P. Courel, P. Trocellier, M. Mosbah, N. Toulhoat, J. Gosset, P.
Massiot and D. Piccot, Nucl. Instr. Meth. B54 (1991) 429.
- J.D. MacArthur and X.-P. Ma, J. PIXE 1 (1991) 311.
- C.G. Ryan and W.L. Griffin, "The Nuclear Microprobe as a tool in
geology and mineral exploration", Nucl. Instr. Meth. B77 (1993) 381-398.
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