## Interactions of High Energy Particles with Nuclei |

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Page 18

From our discussion of the components of otot ( oel , odt , O PROD ) it follows that the measurements of otot may be a good way of finding out whether the inelastic shadowing ( or inelastic screening )

From our discussion of the components of otot ( oel , odt , O PROD ) it follows that the measurements of otot may be a good way of finding out whether the inelastic shadowing ( or inelastic screening )

**corrections**are important at very ... Page 19

Let us consider first the Coulomb

Let us consider first the Coulomb

**corrections**for heavy nuclei . One can , in principle , use the individual amplitudes which have Coulomb interactions built into them ( this very tedious calculation has been done , e.g. , in refs . Page 22

These two factors make Coulomb

These two factors make Coulomb

**corrections**insignificant in dopt / d2 . How important are the details of the target nucleus wave function ? Not very important . The most important are general characteristics : density distributions ... Page 23

SA ) = exp ( iA.r ) m ' ( A ; si ' ... sa ' ) ( 3.8 ) Then we can compute the

SA ) = exp ( iA.r ) m ' ( A ; si ' ... sa ' ) ( 3.8 ) Then we can compute the

**correction**factor to M = ( M ( A ; 81 ... SA ) ) assuming the wave function to be in the form of a product of the c.m. wave function and the internal wave ... Page 24

Hence if we can factor out the c.m. wave function from the product Vo = II ; $ ; ( r ; ) we can stick to calculating M with y , but we have to multiply it by a

Hence if we can factor out the c.m. wave function from the product Vo = II ; $ ; ( r ; ) we can stick to calculating M with y , but we have to multiply it by a

**correction**factor : ( Q ( r ) | exp ( iA.r ) | R ( r ) ) - 1 .### What people are saying - Write a review

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absorption additivity analysis approximately assume attenuation beam Bureau of Standards charge coherent collision complete components compute consider contribution corrections Coulomb Coulomb interactions coupling cross section db exp depend describe deuteron diffractive production processes discussed effects elastic scattering elastic scattering amplitude equation example excited existence exp ia.b 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 National Bureau Note nuclear nuclear targets nuclei nucleon numbers objects obtained parameters phase shifts photon photoproduction physical position possible present problem profiles regeneration shadowing single Standards step strong structure technical vector meson wave function