Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Results 1-5 of 14
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 of phase anomalous magnetic moment ú approximately assume attenuation b+½s beam Bureau of Standards coherent diffractive production collision Compton scattering compute Coulomb interactions Czyż d³r db exp i▲·b deuteron diagonalization diffractive production processes diffractive scattering discussed double scattering elastic scattering amplitude electromagnetic equation example excited experiments factor Feynman diagrams formula four-momentum Glauber model hadrons Hence high energy limit incident particle incident wave inelastic shadowing Interactions of High invariant mass K mesons multiple scattering National Bureau neutrino neutrons ññ Note nuclear matter nuclear targets nuclei nucleon obtained optical theorem parameters phase shifts photon photoproduction of vector physical pion production amplitude profiles quantum numbers regeneration Řº shadowing effects single scattering spin strongly interacting target nucleus total cross section vector meson VMD model wave function γν Σ Σ