Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 2
... - tering amplitude . The expression 1 - eix ; ( b ) = y ; ( b ) is called the profile of the jth nucleon , incident particle collision . Assuming x ( b ) = = Σx ; ( b - s ; ) and assuming that the particle goes through the target so 2.
... - tering amplitude . The expression 1 - eix ; ( b ) = y ; ( b ) is called the profile of the jth nucleon , incident particle collision . Assuming x ( b ) = = Σx ; ( b - s ; ) and assuming that the particle goes through the target so 2.
Page 5
... we end up with an expression which is virtually the same as in the case of the Schrödinger equation : a ( -i + ev ) p = 0 dz whose solution ❤ = u ( k ) exp k ) exp ( -ie [ ' _ da'V ( b , a ' ) ) 00 gives where u ( k ) is a four - 5.
... we end up with an expression which is virtually the same as in the case of the Schrödinger equation : a ( -i + ev ) p = 0 dz whose solution ❤ = u ( k ) exp k ) exp ( -ie [ ' _ da'V ( b , a ' ) ) 00 gives where u ( k ) is a four - 5.
Page 15
... the particle 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.
... the particle 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
... expression x . = Σ ; x ;. ) . This assumption is , of course , obvious in potential scattering . 1 x ( b ) ¦ = - • + ∞ 00 dz [ V . ( b , z ) + V . ( b , z ) ] = x . ( b ) + xc ( b ) db bJo ( Ab ) { 1— exp [ i ( x . ( b ) + x . ( b ) ...
... expression x . = Σ ; x ;. ) . This assumption is , of course , obvious in potential scattering . 1 x ( b ) ¦ = - • + ∞ 00 dz [ V . ( b , z ) + V . ( b , z ) ] = x . ( b ) + xc ( b ) db bJo ( Ab ) { 1— exp [ i ( x . ( b ) + x . ( b ) ...
Page 20
... expression for the complete amplitude by adding and subtracting a Coulomb point charge amplitude : M = ik = 00 db bJ , ( Ab ) [ 1 − exp ( ix . ” ( b ) ) ] + ik [ * db bJo ( Ab ) exp [ ix . ” ( b ) + ix . ( b ) ] · Mc ( P ) + ik 5 00 0 ...
... expression for the complete amplitude by adding and subtracting a Coulomb point charge amplitude : M = ik = 00 db bJ , ( Ab ) [ 1 − exp ( ix . ” ( b ) ) ] + ik [ * db bJo ( Ab ) exp [ ix . ” ( b ) + ix . ( b ) ] · Mc ( P ) + ik 5 00 0 ...
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 |