Spelling suggestions: "subject:"differential crosssections"" "subject:"differential crossections""
1 |
Scattering of 310-Mev positive pions by protons experiments and analysis /Rogers, Ernest H. January 1962 (has links)
Thesis (Ph.D.)--University of California, Berkeley, 1962. / "UC-34 Physics" -t.p. "TID-4500 (17th Ed.)" -t.p. Includes bibliographical references (p. 61-62).
|
2 |
A test of isotopic spin conservation in strong interactions from an experimental limit on [sigma](d + d [right arrow] He⁴+[pi]⁰)Pripstein, Morris. January 1962 (has links)
Thesis (Ph.D.)--University of California, Berkeley, 1962. / "UC-34 Physics" -t.p. "TID-4500 (17th Ed.)" -t.p. Includes bibliographical references (p. 67-69).
|
3 |
Polarization and differential cross sections in proton-proton and proton-nucleus scatterings at 730 MeVMcManigal, Paul G. January 1963 (has links)
Thesis--University of California, Berkeley, 1963. / "UCRL-10637." "UC-34 Physics" -t.p. "TID-4500 (19th Ed.)" -t.p. Includes bibliographical references (p. 64-65).
|
4 |
Regge poles and asymptotic behavior in the analytic continuation of the pion-nucleon scattering amplitudeSingh, Virendra. January 1962 (has links)
Thesis (Ph.D.)--University of California, Berkeley, 1962. / "UC-34 Physics" -t.p. "TID-4500 (17th Ed.)" -t.p. Includes bibliographical references (p. 59-60).
|
5 |
Differential cross sections for elastic scattering of positive pi mesons on protons in the energy region 500 to 1600 MeVHelland, Jerome A. January 1962 (has links)
Thesis--University of California, Berkeley, 1962. / "UC-34 Physics" -t.p. "TID-4500 (17th Ed.)" -t.p. Includes bibliographical references (p. 87-88).
|
6 |
Elastic scattering of 30-Mev protonsLeahy, John. January 1956 (has links)
Thesis--University of California, Berkely. / "Physics Distribution." Includes bibliographical references (p. 37-38). 45
|
7 |
Production of Li, Be and B nuclei in the interaction of 12C with 12C at incident energies of 200 and 400 MeV /Mira, Joele Paulus. January 2008 (has links) (PDF)
Thesis (M.Sc.) - University of the Western Cape, 2008. / Bibliography: leaves 97-101.
|
8 |
The semiclassical S-matrix theory of three body Coulomb break-upChocian, Peter January 1999 (has links)
No description available.
|
9 |
Open charm production in deep inelastic diffractive ep scattering at HERACole, Joanne Elise January 1999 (has links)
No description available.
|
10 |
Shape functions in calculations of differential scattering cross-sectionsJohansson, Anders January 2010 (has links)
<p>Two new methods for calculating the double differential scattering cross-section (DDSCS) in electron energy loss spectroscopy (EELS) have been developed, allowing for simulations of sample geometries which have been unavailable to earlier methods of calculation. The new methods concerns the calculations of the <em>thickness function</em> of the DDSCS. Earlier programs have used an analytic approximation of a sum over the lattice vectors of the sample that is valid for samples with parallel entrance and exit surfaces.The first of the new methods carries out the sum explicitly, first identifying the unit cells illuminated by the electron beam, which are the ones needed to be summed over. The second uses an approach with Fourier transforms, yielding a final expression containing the <em>shape amplitude</em>, the Fourier transform of the <em>shape function</em> defining the shape of the electron beam inside the sample. Approximating the shape with a polyhedron, one can quickly calculate the shape amplitude as sums over it’s faces and edges. The first method gives fast calculations for small samples or beams, when the number of illuminated unit cells is small. The second is more efficient in the case of large beams or samples, as the number of faces and edges of the polyhedron used in the calculation of the shape amplitude does not need to be increased much for large beams. A simulation of the DDSCS for magnetite has been performed, yielding diffraction patterns for the L<sub>3</sub> edge of the three Fe atoms in its basis.</p>
|
Page generated in 0.1283 seconds