Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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... field of high energy diffractive scattering and production processes . In addition to reviewing some well - known material there is much here that is new , both in content and form of presentation . The material presented here is also ...
... field of high energy diffractive scattering and production processes . In addition to reviewing some well - known material there is much here that is new , both in content and form of presentation . The material presented here is also ...
Page 4
... field ( notation from Bjorken and Drell [ S7 ] ) : iv - eA- ке ( i - c + Fm ) = 0 , 4m where y ° A ° -y . A , i ке ... fields ( E , B ) in terms of which 1⁄2KoμF = -21⁄2K ( σ01 Ex + σ02E + 003 E2 ) where Σ = ( 023 , 31 , σ12 ) 023 ...
... field ( notation from Bjorken and Drell [ S7 ] ) : iv - eA- ке ( i - c + Fm ) = 0 , 4m where y ° A ° -y . A , i ке ... fields ( E , B ) in terms of which 1⁄2KoμF = -21⁄2K ( σ01 Ex + σ02E + 003 E2 ) where Σ = ( 023 , 31 , σ12 ) 023 ...
Page 7
... field ( at two different positions ) are , in general , noncommuting operators and there is no way of adding phase shifts ( or , equivalently , multiplying profiles ) . We can also see that the physical reason for this phenomenon is the ...
... field ( at two different positions ) are , in general , noncommuting operators and there is no way of adding phase shifts ( or , equivalently , multiplying profiles ) . We can also see that the physical reason for this phenomenon is the ...
Page 8
... field at two different points . Then 0 , \ i [ ( x − x1 ) + i ( y — yı ) ] , a = a1 + a2 = K Vi ( r- Ir - ri - ri D ) ' 0 , + K V2r - r2 ) | r - r2 | ---- \ i [ ( x − x2 ) + i ( y — Y2 ) ] , — i [ ( x − x1 ) — i ( y — iyı ) ] ) 0 — i [ ...
... field at two different points . Then 0 , \ i [ ( x − x1 ) + i ( y — yı ) ] , a = a1 + a2 = K Vi ( r- Ir - ri - ri D ) ' 0 , + K V2r - r2 ) | r - r2 | ---- \ i [ ( x − x2 ) + i ( y — Y2 ) ] , — i [ ( x − x1 ) — i ( y — iyı ) ] ) 0 — i [ ...
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... field in which the " principle of additivity of phase shifts " is also violated . Let us consider a vector particle ( hence a very relevant kind of particle to our further analysis ) . Example 2. Scattering of a charged vector meson in ...
... field in which the " principle of additivity of phase shifts " is also violated . Let us consider a vector particle ( hence a very relevant kind of particle to our further analysis ) . Example 2. Scattering of a charged vector meson in ...
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