## Interactions of High Energy Particles with Nuclei |

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Page 1

... and diffractive excitation , ( 5 ) Diffractive production of hadrons in hadron - nucleon collisions , ( 6 ) Shadowing effects in

... and diffractive excitation , ( 5 ) Diffractive production of hadrons in hadron - nucleon collisions , ( 6 ) Shadowing effects in

**inelastic**electron - nucleus scattering , ( 7 ) Shadowing effects in neutrino reactions on nuclei . Page 18

O O O They are the source of the so - called

O O O They are the source of the so - called

**inelastic**screening ( or**inelastic**shadowing ) phenomenon [ 47 ] . In order to include them we have to ascribe some kind of structure to the incident particle . Earlier in these notes we gave ... Page 28

Examples : in QED ; elastic electron ( positron ) scattering from a Coulomb field , Delbrück scattering , Compton scattering , etc. in hadron physics ; all kinds of elastic hadron - hadron scattering do = ƒ ( A2 ) dA2

Examples : in QED ; elastic electron ( positron ) scattering from a Coulomb field , Delbrück scattering , Compton scattering , etc. in hadron physics ; all kinds of elastic hadron - hadron scattering do = ƒ ( A2 ) dA2

**inelastic**... Page 29

Let us compute the elastic and

Let us compute the elastic and

**inelastic**scattering amplitudes . Since the transmitted wave is = n , the wave which goes into scattering and production is ¥ n = nyyλeln + λinelnxe ; But hence ¥ 1 = Ny ¥ n — N2 ¥ ¤ × ¢ z ; λel = ny2 ... Page 31

... In this approximation zero - = ( 1 - nj ) dij + eji ( 1 − nj ) — € ji ( 1 —ni ) . ( Xi | T | X ) = 1 − n zero ( 4.3 ) Hence the absorption parameters n ; are determined by elastic scattering of real particles . The

... In this approximation zero - = ( 1 - nj ) dij + eji ( 1 − nj ) — € ji ( 1 —ni ) . ( Xi | T | X ) = 1 − n zero ( 4.3 ) Hence the absorption parameters n ; are determined by elastic scattering of real particles . The

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