## Interactions of High Energy Particles with Nuclei |

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Page 1

... to learn something about the nature of the ( 3 , 3 ) resonance because the exclusion principle ( due to the many particle structure of the target ) may distort the resonance and this distortion may

... to learn something about the nature of the ( 3 , 3 ) resonance because the exclusion principle ( due to the many particle structure of the target ) may distort the resonance and this distortion may

**depend**on its internal structure . Page 11

Otherwise one should realize that k ,

Otherwise one should realize that k ,

**depends**on 8 which sits in the Fourier transform of the shadow . Hence , away from the scatterer , one would guess the following shape of the wave ( compare D. R. Yennie article in [ S3 ] ) : 1 eik ... Page 13

( b – 8,16 ) +5,6 " ) 6 ) - *** , = [ + d ? s , ( $ ) p < ( " ) ( 81 ) ¥ ; ( b 82 ( 0 ) +8 ; ( ) ) ( it does not

( b – 8,16 ) +5,6 " ) 6 ) - *** , = [ + d ? s , ( $ ) p < ( " ) ( 81 ) ¥ ; ( b 82 ( 0 ) +8 ; ( ) ) ( it does not

**depend**on l when all nucleons are " equivalent " ) = ýji ( b + s ; ( ( ) ) Then the ... Page 15

If these geometric characteristics do not

If these geometric characteristics do not

**depend**on energy , one gets the total cross section ( from the optical theorem ) which is energy independent . So , it seems to be difficult to reconcile this model with the recent evidence for ... Page 26

... 2т which operator , in this approximation , does not

... 2т which operator , in this approximation , does not

**depend**on spins . So , if not for the S12 term in ( 3.10 ) , we would have ( mm m ' ) = 0 for m #m ' . In fact the ( mmm ' ) contributions are indeed the most important but they ...### 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