Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
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Page 1
... beams ) . Nevertheless , one still hopes to be able to learn something new , for example about short range nucleon correlation functions in target nuclei or about the pres- ence of resonances in nuclear ground states [ 3 , 4 ] -just to ...
... beams ) . Nevertheless , one still hopes to be able to learn something new , for example about short range nucleon correlation functions in target nuclei or about the pres- ence of resonances in nuclear ground states [ 3 , 4 ] -just to ...
Page 15
... gets removed from the incident beam is 1— | 1 — y ( b ) | 2 = 2 Rey ( b ) ( b ) 2 ( at the impact parameter b ) . Notice that here we use the same expression as in the following paragraphs : we identify 1–7 with y 15.
... gets removed from the incident beam is 1— | 1 — y ( b ) | 2 = 2 Rey ( b ) ( b ) 2 ( at the impact parameter b ) . Notice that here we use the same expression as in the following paragraphs : we identify 1–7 with y 15.
Page 19
... beam of particles . For isospin zero targets ( He , 160 ) , if one finds no difference between the elastic cross section for and it implies that there is no real part in the π - nucleus elastic scattering strong interaction phase shift ...
... beam of particles . For isospin zero targets ( He , 160 ) , if one finds no difference between the elastic cross section for and it implies that there is no real part in the π - nucleus elastic scattering strong interaction phase shift ...
Page 22
... beam ( ~ 50 MeV ) , hence they sum over all nuclear excitations ( without producing mesons , however ) . The cross section for such " inclusive " processes is do sc ΦΩ = n n ik Σ db exp ( i △ · b ) ( Y2 | Ã ( b ; 81 . . . 8. ) | Yo ) ...
... beam ( ~ 50 MeV ) , hence they sum over all nuclear excitations ( without producing mesons , however ) . The cross section for such " inclusive " processes is do sc ΦΩ = n n ik Σ db exp ( i △ · b ) ( Y2 | Ã ( b ; 81 . . . 8. ) | Yo ) ...
Page 31
... beam and its scattering ( elastic ) properties are known reasonably well . The trouble is with the outgoing objects ; e.g. , when 3 are produced in the → 3 reaction : are then its n's given by the absorption of 37 in the target ? In ...
... beam and its scattering ( elastic ) properties are known reasonably well . The trouble is with the outgoing objects ; e.g. , when 3 are produced in the → 3 reaction : are then its n's given by the absorption of 37 in the target ? In ...
Common terms and phrases
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 |