Energy loss of light ions channeling in silicon

• Main Author: Melvin, Jonathan David
• Format: Others
• Published: 1974
• Online Access: https://thesis.library.caltech.edu/9258/1/Melvin_JD_1974.pdf; Melvin, Jonathan David (1974) Energy loss of light ions channeling in silicon. Dissertation (Ph.D.), California Institute of Technology. doi:10.7907/WJBG-JE54. https://resolver.caltech.edu/CaltechTHESIS:10292015-095449554 <https://resolver.caltech.edu/CaltechTHESIS:10292015-095449554>

<p>Experimental measurements of rate of energy loss were made for protons of energy .5 to 1.6 MeV channeling through 1 μm thick silicon targets along the &lt;110&gt;, &lt;111&gt;, and &lt;211&gt; axial directions, and the {100}, {110}, {111}, and {211} planar directions. A .05% resolution automatically controlled magnetic spectrometer was used. The data are presented graphically along with an extensive summary of data in the literature. The data taken cover a wider range of channels than has previously been examined, and are in agreement with the data of F. Eisen, et al., Radd. Eff. 13, 93 (1972).</p> <p>The theory in the literature for channeling energy loss due to interaction with local electrons, core electrons, and distant valence electrons of the crystal atoms is summarized. Straggling is analyzed, and a computer program which calculates energy loss and straggling using this theory and the Moliere approximation to the Thomas Fermi potential, V_TF, and the detailed silicon crystal structure is described. Values for the local electron density Z_loc in each of the channels listed above are extracted from the data by graphical matching of the experimental and computer results.</p> <p>Zeroth and second order contributions to Z_loc as a function of distance from the center of the channel were computed from ∇²V_TF = 4πρ for various channels in silicon. For data taken in this work and data of F. Eisen, et al., Rad. Eff. 13, 93 (1972), the calculated zeroth order contribution to Z_loc lies between the experimentally extracted Z_loc values obtained by using the peak and the leading edge of the transmission spectra, suggesting that the observed straggling is due both to statistical fluctuations and to path variation.</p>