By Y. Manzhur, M. J. Prandolini, K. Potzger, A. Weber, W. -D. Zeitz (auth.), D. R. S. Somayajulu, K. -P. Lieb (eds.)
Proceedings of the Baroda Workshop IWNMS 2004, held in Baroda, India, 10-14 February, 2004
Researchers and graduate scholars drawn to the Mössbauer impression and its purposes will locate this quantity quintessential. the quantity offers the latest advancements within the technique of Mössbauer spectroscopy.
Reprinted from Hyperfine Interactions (HYPE) quantity a hundred and sixty, 1-4
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Additional info for IWNMS 2004: Proceedings of the International Workshop on Nanomaterials, Magnetic Ions and Magnetic Semiconductors Studied Mostly by Hyperfine Interactions (IWNMS 2004) held in Baroda, India, 10–14 February 2004
Sample text
Hydrogen atoms, and loose enough energy in the scattering process such that their range is less than the path out of the sample. The extreme case of backscattering under 180- at a hydrogen atom would actually lead to Rutherford forward scattering with the knocked-on hydrogen atom most probably leaving the sample in the beam direction. Hence, the hydrogen atom content remains unaffected. The cross-section for 180--backscattering, however, is low. For backscattering angles of 90- and below with rapidly rising cross-sections there is a finite chance for further scattering processes.
28 T. BUTZ ET AL. Figure 1. Distribution of the main ferromagnetic impurity Fe found in a C60 polymer sample. As can be seen, Fe is located in small spots at very high concentrations surrounded by large areas of almost pure carbon. The dashed line indicates the outer surface of the sample. The dotted line encircles a Bpure^ region. write magnetic structures with micrometer and sub-micrometer dimensions while Y at the same time Y allowing for impurity analysis via particle induced X-ray emission (PIXE) [3].
12 nC/mm2 measured with Atomic Force Microscopy (AFM) and Magnetic Force Microscopy (MFM) in the tapping/lift mode. , z direction). As can be seen on the left panel, the swelling of the sample in the area of this spot is about 5 nm. For fluences of 75 mC/mm2 we observed a swelling of about 300 nm. The right panel shows the phase shift in degrees as observed with the MFM. Very sharp steps at and near the irradiated spot show up which are not correlated to the topography. This is best illustrated by subjecting the sample to magnetic fields of õ1 kOe THE ROLE OF NUCLEAR NANOPROBES IN INDUCING MAGNETIC ORDERING IN GRAPHITE 35 Figure 7.