Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 12
... describing the collision of two elements is : Yjk ( b − s¿ ( b ) + s , ( @ ) ) . For the sake of simplicity let us take the wave functions of ( a ) and ( b ) in the form of products of single particle wave functions . Let us assume ...
... describing the collision of two elements is : Yjk ( b − s¿ ( b ) + s , ( @ ) ) . For the sake of simplicity let us take the wave functions of ( a ) and ( b ) in the form of products of single particle wave functions . Let us assume ...
Page 14
... describe hadron - hadron scattering in the high energy limit . For example , the limit when A and B become very large was considered [ 13 ] ( compare also [ 12 ] ) : lim M = A , B → ∞ ik 2π d2b exp ( i △ · b ) [ 1– e xp ( − AB ...
... describe hadron - hadron scattering in the high energy limit . For example , the limit when A and B become very large was considered [ 13 ] ( compare also [ 12 ] ) : lim M = A , B → ∞ ik 2π d2b exp ( i △ · b ) [ 1– e xp ( − AB ...
Page 28
... describe diffractive production processes in very close analogy to diffractive dissociation phenomena which are well known in the case of systems where degeneracy exists . Let us start with an example taken from optics . Consider the ...
... describe diffractive production processes in very close analogy to diffractive dissociation phenomena which are well known in the case of systems where degeneracy exists . Let us start with an example taken from optics . Consider the ...
Page 34
... describing the regeneration process K - K , we drew heavily on the known structure of K and K , ° : they are superpositions of K ° and Ko , whose elastic scattering from nucleons is reason- ably well known . 4.1 . Generalizing to Other ...
... describing the regeneration process K - K , we drew heavily on the known structure of K and K , ° : they are superpositions of K ° and Ko , whose elastic scattering from nucleons is reason- ably well known . 4.1 . Generalizing to Other ...
Page 36
... describing elastic scattering we have approximately ( compare eq ( 4.4 ) ) The production amplitude is : p≈p , + p≈π + р . Msi = ( p | T | p ) d1o d1⁄2 TM ” + ( ññ | Т | ññ ) d1⁄2o d ̧ TM ” . Suppose the target is a nucleon , then ( p ...
... describing elastic scattering we have approximately ( compare eq ( 4.4 ) ) The production amplitude is : p≈p , + p≈π + р . Msi = ( p | T | p ) d1o d1⁄2 TM ” + ( ññ | Т | ññ ) d1⁄2o d ̧ TM ” . Suppose the target is a nucleon , then ( p ...
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