Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Results 1-5 of 21
Page 3
... მ 22 hence , neglecting second derivatives of , we obtain the following equation for 4 : 2ikeika = 24 2m dz h2 Veikzy , 24 - dz = 214 Ve where we have used p = kh , v = Р m The amplitude for the particle to scatter from k to 3.
... მ 22 hence , neglecting second derivatives of , we obtain the following equation for 4 : 2ikeika = 24 2m dz h2 Veikzy , 24 - dz = 214 Ve where we have used p = kh , v = Р m The amplitude for the particle to scatter from k to 3.
Page 4
... obtaining the fundamental formula ( 2.1 ) ; the reliability of this formula is of primary importance . The most complete analysis one can perform is presumably to employ the Watson multiple scattering theory , but we shall not present ...
... obtaining the fundamental formula ( 2.1 ) ; the reliability of this formula is of primary importance . The most complete analysis one can perform is presumably to employ the Watson multiple scattering theory , but we shall not present ...
Page 11
... obtain 2ka2 = 2X10 GeVX25 GeV - 2 = 100 fm . Note that ( 3.1 ) gives , as r → ∞ , ( compare D. R. Yennie article in [ S3 ] ) ¥ ( r ) = eik2 + [ ƒ ( ke1 ) / r ] exp ( ikr ) , ( e = component of re2 ) , with f ( ke ) correctly given by ...
... obtain 2ka2 = 2X10 GeVX25 GeV - 2 = 100 fm . Note that ( 3.1 ) gives , as r → ∞ , ( compare D. R. Yennie article in [ S3 ] ) ¥ ( r ) = eik2 + [ ƒ ( ke1 ) / r ] exp ( ikr ) , ( e = component of re2 ) , with f ( ke ) correctly given by ...
Page 21
... obtained by integrating p ( r ) over z . The parameters of x . ( b ) were taken from proton - nucleon scat- tering cross sections . For an ap = -0.33 , σn = 0 , = 38.9 mb ( these parameters are resonable for ~ 20 GeV protons ) , one ...
... obtained by integrating p ( r ) over z . The parameters of x . ( b ) were taken from proton - nucleon scat- tering cross sections . For an ap = -0.33 , σn = 0 , = 38.9 mb ( these parameters are resonable for ~ 20 GeV protons ) , one ...
Page 30
... obtained the result completely analogous to the one obtained for the optical diffractive production : for ij the production amplitude is proportional to the difference in absorptions of the i , j components . This is a very general ...
... obtained the result completely analogous to the one obtained for the optical diffractive production : for ij the production amplitude is proportional to the difference in absorptions of the i , j components . This is a very general ...
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 |
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