## Interactions of High Energy Particles with Nuclei |

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Page 7

Each infinitesimal

Each infinitesimal

**step**x ( z + Az ) – x ( z ) = iAzK ( 01.31 - idi.E10 , ) x ( 2 ) , x ( 2+ Az ) = eiA : K ( * ) x ( 2 ) , ) should be applied in order of increasing z's . That is what { ... } + means . In any case , the additivity ... Page 18

But as long as we construct the profiles of the target nucleus from profiles of elastic scattering , the processes like the one shown in figure 7 ( with excited states of the projectile present at intermediate

But as long as we construct the profiles of the target nucleus from profiles of elastic scattering , the processes like the one shown in figure 7 ( with excited states of the projectile present at intermediate

**steps**) are excluded . Page 35

0 Summing up : Our procedure for evaluating diffractive production in the limit of very high energy consists of two

0 Summing up : Our procedure for evaluating diffractive production in the limit of very high energy consists of two

**steps**: ( i ) Find a " plausible ” model and identify the components of the incident and outgoing systems . Page 43

... -Ev rv Then M ( y = + ) = m ( = V ) πα Σ ( γ - V ) = V γν But νπα M ( 9V ) = M ( VV ) γν 4 Note that restricting the high energy photon - nucleus interaction to only vector meson interactions ( VMD model ) is a very drastic

... -Ev rv Then M ( y = + ) = m ( = V ) πα Σ ( γ - V ) = V γν But νπα M ( 9V ) = M ( VV ) γν 4 Note that restricting the high energy photon - nucleus interaction to only vector meson interactions ( VMD model ) is a very drastic

**step**. Page 55

Let us make this extension explicitly and obtain the so - called " one

Let us make this extension explicitly and obtain the so - called " one

**step**” model for diffractive production of hadrons in hadronnucleus collisions . In this “ one**step**” process , the production takes place on a nucleon inside the ...### What people are saying - Write a review

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### Common terms and phrases

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