Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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... of this cooperation is reflected , however , not only in published papers , but in numerous un- published notes as well as in these lectures themselves . L. C. Maximon Interactions of High Energy Particles with Nuclei * W. Czyż iii.
... of this cooperation is reflected , however , not only in published papers , but in numerous un- published notes as well as in these lectures themselves . L. C. Maximon Interactions of High Energy Particles with Nuclei * W. Czyż iii.
Page 1
... notes the interactions of various different particles with nuclear targets are to be con- sidered . Of course , we cannot cover all problems related to the interactions of hadrons , photons , and electrons ( virtual photons ) with ...
... notes the interactions of various different particles with nuclear targets are to be con- sidered . Of course , we cannot cover all problems related to the interactions of hadrons , photons , and electrons ( virtual photons ) with ...
Page 5
... ( note that ( 1 + a3 ) ( 1— α3 ) = a32 = 0 ) 0 = = · ¿ 1⁄2 ( 1 + α3 ) α1 • ▽ 1 — ¿ 1⁄2 ( 1 + α3 ) α3 + 11⁄2 ( 1 + α3 ) ẞm dz −K1⁄2 ( 1 + as ) ß ( Σ · B − ia · E ) + eV1⁄2 ( 1 + a3 ) | ¢ . ❤ . But in the limit E → ∞ , ( 1 + α3 ) α ...
... ( note that ( 1 + a3 ) ( 1— α3 ) = a32 = 0 ) 0 = = · ¿ 1⁄2 ( 1 + α3 ) α1 • ▽ 1 — ¿ 1⁄2 ( 1 + α3 ) α3 + 11⁄2 ( 1 + α3 ) ẞm dz −K1⁄2 ( 1 + as ) ß ( Σ · B − ia · E ) + eV1⁄2 ( 1 + a3 ) | ¢ . ❤ . But in the limit E → ∞ , ( 1 + α3 ) α ...
Page 7
... Note that " compositeness " of the incident particle is responsible for the existence of more than one channel . For instance , the presence of an anomalous magnetic moment can be looked upon as a mark of " compositeness . " Suppose Anm ...
... Note that " compositeness " of the incident particle is responsible for the existence of more than one channel . For instance , the presence of an anomalous magnetic moment can be looked upon as a mark of " compositeness . " Suppose Anm ...
Page 8
... Note that since the z dependence is outside the spinor matrix this does commute at different z's : [ a ( b , z ) , a ( b , z ' ) ] = 0 . Suppose , however , we have two sources of Coulomb field at two different points . Then 0 , \ i ...
... Note that since the z dependence is outside the spinor matrix this does commute at different z's : [ a ( b , z ) , a ( b , z ' ) ] = 0 . Suppose , however , we have two sources of Coulomb field at two different points . Then 0 , \ i ...
Common terms and phrases
absorption additivity analysis approximately assume attenuation beam coherent collision complete components compute consider contribution corrections Coulomb Coulomb interactions coupling cross section db exp db exp i▲·b depend describe deuteron diffractive production processes discussed effects elastic scattering elastic scattering amplitude equation example excited existence experimental experiments expression fact factor field final formula forward given gives Glauber ground hadrons Hence high energy limit important incident particle inelastic initial Institute interactions introduce magnetic mass measurement momentum transfer multiple scattering Note nuclear nuclear targets nuclei nucleon numbers objects obtained parameters phase shifts photon photoproduction physical position possible problem profiles regeneration shadowing single Standards step strong structure technical vector meson wave function weak
Bibliographic information
| Title | Interactions of High Energy Particles with Nuclei Volume 139 of NBS monograph |
| Author | Wiesław Czyż |
| Publisher | National Bureau of Standards, 1975 |
| Original from | the University of Michigan |
| Digitized | 21 Nov 2007 |
| Length | 69 pages |
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