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Positron Annihilation Methods by r-Rays Produced in Laser-Induced Compton-Backscattering

机译:通过激光诱导的康普顿反向散射产生的R射线正电子湮没方法

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Positron annihilation methods are unique and strong tools to investigate materials. However, positrons are usually injected from outside of the samples. Therefore, the samples should be in a vacuum or radioisotopes should be attached. Recently, Selim et al. applied high-energy y-rays (2 MeV) produced by a 6 MeV electron linac to create positrons in thick materials. We have also been trying a similar technique. In our case, high-energy γ-rays (~20 MeV) produced in laser-induced Compton-backscattering are applied to positron creation in samples. The γ-rays do not spread and are not absorbed in air. When you place a sample in the path of the γ-rays, positrons are created in the sample and conventional positron annihilation methods can be applied. Moreover, it is not necessary to place the samples in vacuum and radioisotopes are not required. This means that the measurements of materials such as metals at very high temperature, near or over melting points, will be possible. The details of this method and some examples of experimental results will be introduced.
机译:正电子湮灭方法是调查材料的独特和强大的工具。但是,正水通常从样品外部注射。因此,样品应在真空或放射性同位素中附着。最近,Selim等人。应用高能Y射线(2 MEV)由6MeV电子LINAC产生,以在厚材料中产生正态。我们也一直在尝试一种类似的技术。在我们的情况下,激光诱导的康普顿反向散射中产生的高能γ射线(〜20meV)应用于样品中的正电子创作。 γ射线不会涂抹并且不在空气中被吸收。当您在γ射线的路径中放置样品时,在样品中产生正数,并且可以应用传统的正电子湮灭方法。此外,不需要将样品放置真空,并且不需要放射性同位素。这意味着将可以在可能的情况下测量诸如金属的材料,如熔点在熔点附近或过度熔点。将介绍该方法的细节和实验结果的一些例子。

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