Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 1
... components in such interactions . This article is divided into seven sections : ( 1 ) Introduction , ( 2 ) Description of multiple scat- tering , ( 3 ) Elastic scattering of hadrons from nuclei , ( 4 ) Diffractive dissociation and ...
... components in such interactions . This article is divided into seven sections : ( 1 ) Introduction , ( 2 ) Description of multiple scat- tering , ( 3 ) Elastic scattering of hadrons from nuclei , ( 4 ) Diffractive dissociation and ...
Page 5
... components ( in x , y plane ) are marked 1. Thus , finally , we find a + eV - Kß ( Σ1 · В1 — ¿ α · E ) | p = 0 . Əz ( 2.4 ) So , if the anamalous magnetic moment K = 0 , we end up with an expression which is virtually the same as in the ...
... components ( in x , y plane ) are marked 1. Thus , finally , we find a + eV - Kß ( Σ1 · В1 — ¿ α · E ) | p = 0 . Əz ( 2.4 ) So , if the anamalous magnetic moment K = 0 , we end up with an expression which is virtually the same as in the ...
Page 6
... component spinor because F has to satisfy the relation So , F can be taken in the form ( 1 - α3 ) F = 0 , a Χ F ... components of the spinor x ) . Call In general a ( x , y , z ) = K ( 81.B1 - io1 E10 ) . [ a ( x , y , z ) , A ( x ...
... component spinor because F has to satisfy the relation So , F can be taken in the form ( 1 - α3 ) F = 0 , a Χ F ... components of the spinor x ) . Call In general a ( x , y , z ) = K ( 81.B1 - io1 E10 ) . [ a ( x , y , z ) , A ( x ...
Page 11
... component of re2 ) , with f ( ke ) correctly given by the inverse of y ( b ) . One can see this by shifting the origin of integra- tion to ke1 : Then and 1 8 = ke1 + q ( we introduce a new variable q ) . z√k2 - d2 + 8.b≈kr- 1 q2r 2 k ...
... component of re2 ) , with f ( ke ) correctly given by the inverse of y ( b ) . One can see this by shifting the origin of integra- tion to ke1 : Then and 1 8 = ke1 + q ( we introduce a new variable q ) . z√k2 - d2 + 8.b≈kr- 1 q2r 2 k ...
Page 12
... COMPONENTS ( b ) ( 0 ) O B COMPONENTS The profile 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 ...
... COMPONENTS ( b ) ( 0 ) O B COMPONENTS The profile 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 ...
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 |
| Export Citation | BiBTeX EndNote RefMan |