Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
Indirect determination of Li via 74Ge(n,γ)75mGe activation reaction induced by neutrons from 7Li(p,n)7Be reaction
Introduction
Proton induced nuclear reactions namely 7Li(p,p′γ)7Li, 7Li(p,γ)8Be and 7Li(p,α)4He are widely used for the analysis of Li in materials [1]. Among these, 7Li(p,p′γ)7Li is often the reaction of choice for the determination of the element by the particle induced γ-ray emission (PIGE) technique. The analysis is generally performed using a 1–4 MeV proton beam and involves the measurement of the 478 keV prompt γ-rays by a high purity germanium (HPGe) detector. The reaction has a high cross-section and is largely free from interferences: except B [10B(p,αγ)7Be → 7Li] and Mn [55Mn(p,nγ)55Fe] no other element interferes in the analysis. As a result, it enables a sensitive determination of Li, in many cases down to ppm levels.
The reactions 7Li(p,γ)8Be (Q = 17.3 MeV) and 7Li(p,α)4He (Q = 17.3 MeV), on the other hand, are mainly used for depth profile measurements [2], [3]. The typical depth resolutions of these reactions are about 0.15 and 1 μm, respectively. 7Li(p,n)7Be (Q = −1.644 MeV) is another important reaction induced by protons. It is a well-studied nuclear reaction, particularly as a source of (monoenergetic) neutrons. However, it has been used only on few occasions for the determination of Li. In one such application, Sellschop et al. utilized the reaction in the analysis of diamond [4]. They reported a detection sensitivity of about 2 ppm but did not provide any experimental or analytical details. In yet another application, Sippel and Glover analysed sedimentary rocks using a BF3 counter for neutron detection and achieved a detection sensitivity of about 100 ppm [5]. Meanwhile, it is important to note that 7Be formed in the reaction decays by electron capture (EC) (t1/2 = 53.3 d) emitting 478 keV γ-rays. The activity of 7Be produced under irradiation conditions generally employed in the analysis of Li by PIGE is very low, and therefore the 478 keV γ-rays detected during such measurements are overwhelmingly prompt. The reaction 7Li(p,n)7Be → 7Li, however, is extensively used for the determination of Li by charged particle activation analysis (CPAA) [6].
In this paper we present a novel approach for the determination of Li which combines the 7Li(p,n)7Be reaction and neutron activation analysis (NAA) involving the 74Ge(n,γ)75mGe reaction. In a typical PIGE experimental set up, neutrons produced in a thick, Li containing target as a consequence of the 7Li(p,n)7Be reaction, initiate the 74Ge(n,γ)75mGe reaction in a HPGe detector. 75mGe (t1/2 = 47.7 s) emits 139 keV γ-rays which are measured by the detector thereby facilitating the determination of Li. The report includes studies on interferences, compares the results with those obtained by PIGE involving the 7Li(p,p′γ)7Li reaction and shows that the 74Ge(n,γ)75mGe reaction occurring in the HPGe detector can be advantageously utilized to monitor even low fluxes of neutrons as well.
Section snippets
Kinematics of 7Li(p,n)7Be reaction
The 7Li(p,n)7Be nuclear reaction is endoergic (Q = −1.644 MeV) and therefore has a threshold (Eth) of 1.88 MeV. A kinematical consideration of the reaction shows that (a) at a proton energy (Ep) = Eth, neutrons are emitted only at 0° (laboratory co-ordinates) with an energy of 29.7 keV, (b) up to Ep ⩽ 1.92 MeV, neurons are emitted within a small forward cone whose angle increases with Ep and (c) for Ep > 1.92 MeV, neutron emission is energetically allowed in all directions. Fig. 1 provides kinematic
Irradiation and γ-ray detection
The measurements were performed using the 3 MV Tandetron (HVEE, Europa) at the Centre. Thick pellets containing 368–2130 ppm Li were used as targets. These were prepared by mixing appropriate amounts of lithium fluoride or lithium carbonate in high purity graphite powder. Adequate care was taken to ensure homogeneous distribution of Li in the graphite powder. The targets were irradiated with the 800–3000 keV proton beam. The beam current over a spot about 4 mm in diameter was, 5–20 nA for the
Spectral features and origin of γ-rays
Fig. 3 shows the prompt γ-ray spectrum acquired on irradiating a target containing about 2130 ppm Li (as LiF) with a 3.0 MeV proton beam. The peak at 478 keV arises from the 7Li(p,p′γ)7Li reaction while the one at 429 keV from the 7Li(p,nγ)7Be reaction. Short lifetime of the de-exciting state and high recoil of the light nuclei cause appreciable broadening of the 478 keV peak. The spectrum also consists of strong peaks at 110 and 197 keV that represent γ-rays from the 19F(p,p′γ)19F reaction. In
Conclusion
7Li(p,n)7Be (Eth = 1.88 MeV) is one among several reactions induced simultaneously by a proton beam in a Li-containing target. In a typical PIGE experimental set up, neutrons from this reaction induce the 74Ge(n,γ)75mGe activation reaction (Eγ = 139 keV; t1/2 = 47.7 s) in the Ge crystal of a high purity Ge detector. The measurement of the 75mGe activity thus produced is used to determine Li in a wide, percentage to ppm, concentration range. Apart from sensitivity, rapidity and selectivity are the two
Acknowledgements
The authors thank Dr. T. Mukharjee, Director, Chemistry group, BARC for his support. We also acknowledge useful discussions with Dr. J. Arunachalam, Head, NCCCM and Dr. D.P. Chowdury, ACD, VECC, Kolkatta.
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