## Interactions of High Energy Particles with Nuclei |

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**Consider**the case when one " elementary ” particle scatters from a " composite " nucleus . In this case the profile is ( T ) = ( Vol 1 ( b ; sı ... 8. ) | V. ) , 0 and we can write the same relations as before : OtoT = | xb | ( T ) ? Page 18

... corrections for the c.m. motion which are important for light nuclei but unimportant for heavy ones . Let us

... corrections for the c.m. motion which are important for light nuclei but unimportant for heavy ones . Let us

**consider**first the Coulomb corrections for heavy nuclei 18 O ... Page 19

Let us

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

In order to make this fact more plausible , let us

In order to make this fact more plausible , let us

**consider**a collection of neutrons and protons which do not screen each other . Then , we would have dopt d22 ī N | fn ( A ) 12 + 218p ( A ) 12 . no screening One may suspect the ... Page 23

When we want to discuss light nuclei we have to

When we want to discuss light nuclei we have to

**consider**carefully the motion of the center of mass . Take , for example , a deuteron : here taking into account the c.m. motion is trivially accomplished by using the wave functions of ...### 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