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 depend on its internal structure .
... 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 , depends on d 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 ...
Otherwise one should realize that k , depends on d 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
... +8 ; ( « ) ) = Ỹji ( b + s , ( a ) ) Then the formula ( 3.2 ) reduces to ( 3.3 ) : M = = ik 2π ik - 2π , ( it does not depend on 7 when all nucleons are " equivalent " ) đ3b exp ( i △ · b ) [ d23⁄4 ̧ ...
... +8 ; ( « ) ) = Ỹji ( b + s , ( a ) ) Then the formula ( 3.2 ) reduces to ( 3.3 ) : M = = ik 2π ik - 2π , ( it does not depend on 7 when all nucleons are " equivalent " ) đ3b exp ( i △ · b ) [ d23⁄4 ̧ ...
Page 15
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 ...
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
... in this approximation , does not depend on spins . So , if not for the S12 term in ( 3.10 ) , we would have ( m | M | m ' ) = 0 for mm ' . In fact the ( m | | m ' ) contributions are indeed the most important but they always lead to ...
... in this approximation , does not depend on spins . So , if not for the S12 term in ( 3.10 ) , we would have ( m | M | m ' ) = 0 for mm ' . In fact the ( m | | m ' ) contributions are indeed the most important but they always lead to ...
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absorption additivity analysis approximately assume attenuation beam coherent collision complete components compute consider contribution corrections Coulomb Coulomb interactions coupling cross section db exp db exp i▲·b depend describe deuteron diffractive production processes discussed effects elastic scattering elastic scattering amplitude equation example excited existence 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 Note nuclear nuclear targets nuclei nucleon numbers objects obtained parameters phase shifts photon photoproduction physical position possible problem profiles regeneration shadowing single Standards step strong structure technical vector meson wave function weak
Bibliographic information
| Title | Interactions of High Energy Particles with Nuclei Volume 139 of NBS monograph |
| Author | Wiesław Czyż |
| Publisher | National Bureau of Standards, 1975 |
| Original from | the University of Michigan |
| Digitized | 21 Nov 2007 |
| Length | 69 pages |
| Export Citation | BiBTeX EndNote RefMan |