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Nuclear Resonaynce Vibrational Spectroscopy

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X-Ray Spectroscopy with Synchrotron Radiation

Part of the book series: Biological and Medical Physics, Biomedical Engineering ((BIOMEDICAL))

Abstract

We learned in Chap. 9 that Mössbauer spectroscopy and nuclear forward scattering rely on the zero-phonon, recoil-free fraction, as determined by the Lamb-Mössbauer factor—fLM. In the Mössbauer experiment, the intensity is reduced by this factor, so that the observed cross section is reduced from the total cross section according to σ(0) ~ (π/2) σN fLM. However, there is a “sum rule” that states that the integrated cross section for a nuclear transition remains the same [478]. So, where does this missing intensity go?

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Authors and Affiliations

  1. Advanced Light Source Professor emeritus, University of California, Davis, CA, USA

    Stephen P. Cramer

  2. Senior Research Scientist, SETI Institute, Mountain View, CA, USA

    Stephen P. Cramer

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  1. Stephen P. Cramer
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Cramer, S.P. (2020). Nuclear Resonaynce Vibrational Spectroscopy. In: X-Ray Spectroscopy with Synchrotron Radiation. Biological and Medical Physics, Biomedical Engineering. Springer, Cham. https://doi.org/10.1007/978-3-030-28551-7_10

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