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Gamma holography from multiple scattering

机译:来自多重散射的伽马全息术

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Since the introduction of heterodyne methods for synchrotron radiation (Cousesement et al. in Phys. Rev. B 54:16003, 1996; Callens et al. in Phys. Rev. 67:104423, 2003) one observes interferences between two scattering amplitudes; the scattering amplitude of resonant nuclei in a reference sample and the scattering amplitude of nuclei in the sample under investigation. Theses interferences can easily been observed as resonances in velocity spectra when one uses a time integrated method. They can also been observed as quantum beats, when one would use the time differential method. For both methods it is important that one uses a reference sample and therefore both methods disserved the name “heterodyne methods.” As theses interferences are a product of two scattering amplitudes, the amplitude of a wave scattered form the investigated sample can be known with its phase. But it is assumed that the reference wave is known in advance by a proper choice of the reference sample. At first sight it is very likely that multiple scattering would add more complexity but in this paper it is claimed that on the contrary it provide a bonus, especially for single crystals. It provokes only a line broadening and a line shift of the resonances in the velocity spectra (or a change in the damping and frequency of the quantum beats when the time spectra are registered). Moreover these changes in the line shapes can easily be measured and they provide all the information needed to reconstruct a 3-D picture of the atomic arrangement of resonant nuclei and moreover they distinguish between different hyperfine sites. The method may be more practical for measurements on synchrotron radiation but it does also apply to velocity spectra obtained from resonant scattering with strong sources. The use of radioactive sources suffer from the disadvantage of poorer statistics or much longer accumulation times but they enjoy the advantage to be table-top and at-home experiments. As strong sources are now commercially available this possibility to measure not only the hyperfine fields but also the corresponding crystal structure could give a renewed impetus to the investigations with Moessbauer spectrometry, with “at home and table top” instrumentation.
机译:自从引入用于同步加速器辐射的外差方法(Cousesement等人,在Phys。Rev. B 54:16003,1996; Callens等人在Phys。Rev. 67:104423,2003)中以来,人们就观察到了两个散射振幅之间的干扰。参考样品中共振核的散射幅度和所研究样品中核的散射幅度。当人们使用时间积分方法时,这些干扰很容易被观察为速度谱中的共振。当人们使用时差方法时,也可以将它们视为量子节拍。对于这两种方法,重要的是要使用参考样品,因此这两种方法都保留了“外差法”的名称。由于这些干扰是两个散射振幅的乘积,因此从被调查样品中散射的波的振幅及其相位可以获知。但是假设通过适当选择参考样本可以事先知道参考波。乍一看,很可能多重散射会增加更多的复杂性,但是在本文中,它声称相反地,它提供了额外的好处,尤其是对于单晶体。它仅引起速度谱中共振的线变宽和线移位(或在记录时间谱时,量子拍的阻尼和频率发生变化)。此外,这些线形变化很容易测量,它们提供了重建共振核原子排列的3-D图片所需的所有信息,而且它们可以区分不同的超精细位点。该方法对于同步加速器辐射的测量可能更实用,但它也适用于从强源共振散射获得的速度谱。放射性源的使用具有统计数据较差或累积时间更长的缺点,但它们具有台式和在家实验的优势。由于现在有大量来源可供使用,因此不仅可以测量超精细场,而且可以测量相应的晶体结构,这可以为使用Moessbauer光谱仪和“家用和台式”仪器进行的研究提供新的动力。

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