Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 1
... forward scattering and production processes ) . Such effects are very well established in the case of hadron scattering and photon - nucleus interactions ; they are not well known in the case of neutrino reactions and very virtual ...
... forward scattering and production processes ) . Such effects are very well established in the case of hadron scattering and photon - nucleus interactions ; they are not well known in the case of neutrino reactions and very virtual ...
Page 20
... y ( b ) is very sharp compared to 1/8 ( hence we limit our- selves to forward scattering processes ) we can approximate y ( b ) ≈y ( 0 ) d ‹ 2 ) ( b ) , hence ik f ( 0 ) = Y ( 0 ) , and 2π απ 2π ix . ( b ) ≈ - N 20.
... y ( b ) is very sharp compared to 1/8 ( hence we limit our- selves to forward scattering processes ) we can approximate y ( b ) ≈y ( 0 ) d ‹ 2 ) ( b ) , hence ik f ( 0 ) = Y ( 0 ) , and 2π απ 2π ix . ( b ) ≈ - N 20.
Page 21
... forward forward scattering ampli- tude ) are defined by fn.p ( 0 ) = ( i + an.p ) kon.p / 4π where on.p are the total cross section for scattering on either neutron or proton . ( Incidentally , one can define an optical potential — ( 1 ...
... forward forward scattering ampli- tude ) are defined by fn.p ( 0 ) = ( i + an.p ) kon.p / 4π where on.p are the total cross section for scattering on either neutron or proton . ( Incidentally , one can define an optical potential — ( 1 ...
Page 22
... forward dip , it is not valid for small △ ) do DT = a dn N | 2 A IS . ( A ) 1a + 2152 ( A ) 1 ] , Ꮓ A where the " effective number of nucleons " is a A · [ d3b p ( b ) e ̄ • Ap ‹ b ) , where σ is an average total hadron - nucleon ...
... forward dip , it is not valid for small △ ) do DT = a dn N | 2 A IS . ( A ) 1a + 2152 ( A ) 1 ] , Ꮓ A where the " effective number of nucleons " is a A · [ d3b p ( b ) e ̄ • Ap ‹ b ) , where σ is an average total hadron - nucleon ...
Page 33
... forward direction where the transmission regeneration ( which comes from a coherent process whose coherence extends over the whole block of matter ) dominates . The amplitude ( neglecting 8 ) is MKL ° → K ‚ ° = 1⁄2 ( Ko | T | Ko ) – 1 ...
... forward direction where the transmission regeneration ( which comes from a coherent process whose coherence extends over the whole block of matter ) dominates . The amplitude ( neglecting 8 ) is MKL ° → K ‚ ° = 1⁄2 ( Ko | T | Ko ) – 1 ...
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