Absorption Measurements of Certain Changes in the Average by Allison S. K., Duane W. PDF

By Allison S. K., Duane W.

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The detailed 27 Al(p,p0 )2 7Al excitation function was obtained in the high resolution proton resonance measurements [17]. The R-matrix fit to the data was shown to be in excellent agreement with the measured points. [18] and [19]. 8. 8 the measured points are in a reasonable mutual agreement as well as in a fair agreement with the retrieved high resolution data, however the fine structure of the excitation function is completely missed both in the sparse points measurements of [19] and in the cross sections derived from a thick target yield [18].

C 15, 518 (1977). [9] A. Nurmela, J. Raisanen and E. Rauhala, Nucl. Instr. and Meth. B 136-138, 77 (1998). [10] I. Bogdanovic Radovic and O. Benka, Nucl. Instr. and Meth. B 174, 25 (2001). K. D. Choi, Nucl. Instr. and Meth. B 174, 33 (2001). F. Gurbich, Nucl. Instr. and Meth. B 136-138, 60 (1998). F. Gurbich, Nucl. Instr. and Meth. B 152, 403 (1999). [14] S. Mazzoni, M. Chiari, L. A. Mando and N. Taccetti, Nucl. Instr. and Meth. B 136-138, 86 (1998); 159, 191 (1999). F. L. Ramos, A. Paul, L. C.

2 MeV. The discrepancy has been thoroughly studied but no reasons for such a deviation of the cross section from Rutherford one was found in the present analysis. Because of the lack of another experimental information an additional measurement was made to clear up the problem ([22]). m. d σ /d Ω θ =170 150 100 Rauhala89 50 Chiari01 Theory 1000 1200 1400 1600 1800 2000 Energy (keV) Figure 8: The 27 Al(p,p0 )2 7Al differential elastic scattering cross section. 9). The cross section for natural silicon is a sum of the cross sections for its three stable isotopes weighted by the relative abundance.

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Absorption Measurements of Certain Changes in the Average Wave-Length of Tertiary X-Rays by Allison S. K., Duane W.


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