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Mossbauer spectroscopy neutron experiments

The spectroscopic techniques that have been most frequently used to investigate biomolecular dynamics are those that are commonly available in laboratories, such as nuclear magnetic resonance (NMR), fluorescence, and Mossbauer spectroscopy. In a later chapter the use of NMR, a powerful probe of local motions in macromolecules, is described. Here we examine scattering of X-ray and neutron radiation. Neutrons and X-rays share the property of being found in expensive sources not commonly available in the laboratory. Neutrons are produced by a nuclear reactor or spallation source. X-ray experiments are routinely performed using intense synclirotron radiation, although in favorable cases laboratory sources may also be used. [Pg.238]

Mossbauer spectroscopy was used in combination with ion implantation in the 1960s, shortly after the Mossbauer effect was discovered. In the earliest days, Mossbauer experiments were performed on ion-implanted sources using particle accelerators and nuclear reactors. In 1965, Ruby and Holland [I] populated the 29.6 keV Mossbauer level in K using the (d, p) reaction on potassium metal. Hafemeister and Brooks Shera [2] performed a similar experiment on K using the thermal neutron capture reaction. Berger et al. [3-5] conducted online Mossbauer studies using the (n, y) reaction of Fe. [Pg.58]

The remainder of this chapter is organized as follows. The next section describes some experimental and application investigations of in-beam Mossbauer spectroscopy using a Mn beam at the RIKEN RIBF. The system used for detecting Mossbauer 7-radiation in in-beam experiments is important. Nagatomo et al. [32] have recently developed a highly sensitive resonance counter based on parallel-plate avalanche and plastic scintillation counters. A new anticoincidence detection system is introduced. Finally, the experimental setup for online Mossbauer spectroscopy using the thermal neutron capture reaction, Fe (n, 7) Fe, and the results obtained are presented in the subsequent section. [Pg.61]

F.6. Mossbauer Spectroscopy F.6.1. Introduction F.6.2. The Mossbauer Spectrum F.6.3. Bulk and Surface Static Studies F.6.4. Superparamagnetic Relaxation in Zero Applied Field F.6.5. Influence of a Large Applied Field F.6.6. Influence of a Medium Applied Field F.6.7. Concluding Remarks F.7. Ferromagnetic Resonance F.8. Neutron Experiments... [Pg.285]

The techniques currently used to study the superparamagnetic relaxation are dc susceptibility is not well defined, estimated to be around 100 s, but it depends on the type of magnetometer and on the measuring procedure), ac susceptiblity (t , = 10 -10 s for experiments at very low frequencies t = 10 -10 s for classical experiments t = 10 —l0 s for measurements at very high frequencies, very difficult to realize, so far), Mossbauer spectroscopy (time window, 10 -10 s for Fe), ferromagnetic resonance (t , = 10 s), and neutron diffraction (time window, 10 -10 s, depending on the type of experiments). [Pg.289]


See other pages where Mossbauer spectroscopy neutron experiments is mentioned: [Pg.269]    [Pg.210]    [Pg.330]    [Pg.66]    [Pg.67]    [Pg.132]    [Pg.258]    [Pg.528]    [Pg.339]    [Pg.327]    [Pg.342]    [Pg.343]    [Pg.397]    [Pg.592]    [Pg.421]    [Pg.168]    [Pg.248]    [Pg.52]   
See also in sourсe #XX -- [ Pg.445 , Pg.446 , Pg.447 , Pg.448 , Pg.449 , Pg.450 , Pg.451 ]




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