## Interactions of High Energy Particles with Nuclei |

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Page 18

If this is so , then the three contributions to otot discussed above do

If this is so , then the three contributions to otot discussed above do

**approximately**exhaust the list of processes contributing to elastic scattering . From our discussion of the components of otot ( oel , odt , O PROD ) it follows ... Page 21

It is amusing that numerically Im M with proper xc is

It is amusing that numerically Im M with proper xc is

**approximately**the same as Re M without xe ! This is true for 208Pb . In general one gets all kinds of intermediate situations . In any case , the influence of the Coulomb interaction ... Page 36

T P Final state : nta = + = d , ** | ñ ) + d2an 17 ) . ñ small admixture In the sense given earlier in these notes , for the purpose of describing elastic scattering we have

T P Final state : nta = + = d , ** | ñ ) + d2an 17 ) . ñ small admixture In the sense given earlier in these notes , for the purpose of describing elastic scattering we have

**approximately**( compare eq ( 4.4 ) ) = a p = p * + pTp . Page 41

Example 3 : Photoprocesses and vector meson dominance : It is now a well established fact that , at high energy , photons exhibit shadowing . The total photo cross sections for complex nuclei vary

Example 3 : Photoprocesses and vector meson dominance : It is now a well established fact that , at high energy , photons exhibit shadowing . The total photo cross sections for complex nuclei vary

**approximately**as A0.9 in the few GeV ... Page 45

In fact one does not need a purely electromagnetic interaction to obtain a contribution ~ A . It could come from a heavy vector boson whose Conclusion : The VMD model is only

In fact one does not need a purely electromagnetic interaction to obtain a contribution ~ A . It could come from a heavy vector boson whose Conclusion : The VMD model is only

**approximately**correct . 2w My2 « R is still short because its ...### 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