Experimental methods available at the Laboratory of Nuclear Analytical Methods

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    Elastic Recoil Detection Analysis

     

    ERDA uses high energy (~1MeV/amu) heavy-ion beams to kinematically recoil and depth profile low atomic number target atoms. The heavy ion projectile only needs to have a greater mass than the target atom. Alpha particles are commonly used to obtain recoil spectrum for hydrogen and its isotopes.

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  • Neutron Depth Profiling

     

    Neutron Depth Profiling (NDP) is an isotope specific, non-destructive nuclear analytical technique. It is used for the measurement of concentration profiles of elements in the near-surface region of solids. The technique, first reported by J. F. Ziegler et al. [J. Appl. Phys., 43 (1972) 3809] in 1972, exploits the existence of prompt exoenergetic non-resonant nuclear reactions of certain light isotopes (see Tab. 1) with low energy (< 10-2 eV) neutrons.


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  • Particle Induced Gamma-Ray

     

    PIGE is a versatile technique, which complements other ion beam techniques (especially PIXE) for sample analysis and non-destructive depth profiling. It is the most common application of nuclear analysis. The PIGE method is mostly based on nuclear reactions (p, g), (p,p´g), (p, a g) induced by MeV protons, where prompt nuclear gamma-rays are produced.

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  • Particle Induced X-Ray Spectroscopy

     

    PIXE is method in which X-ray emission is used for elemental analysis. T he high energetic proton beam excites, due to inner-shell ionization, the emission of characteristic X-rays from the sample atoms. In the true sense, PIXE is not a nuclear technique, since the ionisation of the atoms by the ion beam and the subsequent emission of characteristic X-rays are purely atomic electromagnetic processes.

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  • RBS-channeling

     

    RBS-channeling spectrometry - enables us to investigate crystalline materials. The signal of the impurity and host lattice in RBS spectra is separated by scattering kinematics . The angular yield curve (scan) is obtained by monitoring the yield of the impurity and host lattice along the channeling axis using ion beam impact angle changing. From the angular yield curves of the axial channels in virgin material we obtain the impurity position in the measured cut. In order to determine the lattice position of impurities several relevant crystallographic directions have been selected.

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  • Rutherford Backscattering Spectrometry

    RBS is most commonly used non-destructive nuclear method for elemental depth analysis of nm-to-mm thick films. It involves measurement of the number and energy distribution of energetic ions (usually MeV light ions such He+) backscattered from atoms within the near-surface region of solid targets. From such measurement it is possible to determine, with some limitations, both the atomic mass and concentration of elemental target constituents as a function of depth below the surface.

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