Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
From inside the book
Page 26
... number m . The elastic cross - section is then doel ΦΩ = 1 Σ Σ ( m | M ( △ , s ) | m ′ ) | 2 3 m , m ' with ik M ( A , s ) = d2b exp ( i △ · b ) { 1— exp [ ix , ( b − 1⁄2s ) + ixn ( b + 1⁄2s ) ] } , 2π which operator , in this ...
... number m . The elastic cross - section is then doel ΦΩ = 1 Σ Σ ( m | M ( △ , s ) | m ′ ) | 2 3 m , m ' with ik M ( A , s ) = d2b exp ( i △ · b ) { 1— exp [ ix , ( b − 1⁄2s ) + ixn ( b + 1⁄2s ) ] } , 2π which operator , in this ...
Page 27
... numbers . ) All the other spin effects are presumably not important . ( iii ) Calculations such as the one above , as well as more sophisticated calculations , have always produced cross sections in excellent agreement with experiment ...
... numbers . ) All the other spin effects are presumably not important . ( iii ) Calculations such as the one above , as well as more sophisticated calculations , have always produced cross sections in excellent agreement with experiment ...
Page 28
... numbers are exchanged ) . Examples : in QED ; elastic electron ( positron ) scattering from a Coulomb field , Delbrück scattering , Compton scattering , etc. in hadron physics ; all kinds of elastic hadron - hadron scattering do = ƒ ...
... numbers are exchanged ) . Examples : in QED ; elastic electron ( positron ) scattering from a Coulomb field , Delbrück scattering , Compton scattering , etc. in hadron physics ; all kinds of elastic hadron - hadron scattering do = ƒ ...
Page 31
... [ ( 1 + 8 ) | Ko ) − ( 1 − 8 ) | Ão ) ] ~ — ( | Ko ) — | Ko ) ) = | K. ) | K , ° ) = 1 1 | K2 ° ) = [ ( 1 + 8 ) | Ko ) + ( 1−8 ) | Řo ) ] ~ √2 ( 1+ | 8 | 2 ) ( | Ko ) + | Řo ) ) = | K2o ) , √2 where & is a small complex number , | 8 31.
... [ ( 1 + 8 ) | Ko ) − ( 1 − 8 ) | Ão ) ] ~ — ( | Ko ) — | Ko ) ) = | K. ) | K , ° ) = 1 1 | K2 ° ) = [ ( 1 + 8 ) | Ko ) + ( 1−8 ) | Řo ) ] ~ √2 ( 1+ | 8 | 2 ) ( | Ko ) + | Řo ) ) = | K2o ) , √2 where & is a small complex number , | 8 31.
Page 32
Wiesław Czyż. where & is a small complex number , | 8 | ~ 10 - 3 <<< 1 , which gives a measure of CP nonconservation . | K1 ° ) and | K2 ° ) are eigenstates of CP . Indeed P | Řo ) = | Ko ) . == P | Ko ) = − | Ko ) , C | Ko ) = | Řo ...
Wiesław Czyż. where & is a small complex number , | 8 | ~ 10 - 3 <<< 1 , which gives a measure of CP nonconservation . | K1 ° ) and | K2 ° ) are eigenstates of CP . Indeed P | Řo ) = | Ko ) . == P | Ko ) = − | Ko ) , C | Ko ) = | Řo ...
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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