Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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Page 4
... magnetic moment in a given electromagnetic static field ( notation from Bjorken and Drell [ S7 ] ) : iv - eA- ке ( i - c + Fm ) = 0 , 4m where y ° A ° -y . A , i ке σμν Ξ ( y " y " —yy " ) . Denote K = 2 2m ( izoo and multiply it by y ...
... magnetic moment in a given electromagnetic static field ( notation from Bjorken and Drell [ S7 ] ) : iv - eA- ке ( i - c + Fm ) = 0 , 4m where y ° A ° -y . A , i ке σμν Ξ ( y " y " —yy " ) . Denote K = 2 2m ( izoo and multiply it by y ...
Page 5
... magnetic moment K = 0 , 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 ...
... magnetic moment K = 0 , 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 ...
Page 7
... magnetic moment can be looked upon as a mark of " compositeness . " Suppose Anm ( F , F1 , ... ... ... , r ^ ) = Ĉ q☺ ( r − r ; ) . j1 m Diagonalization should produce a diagonal matrix of the form : S - 1as = = \ { 3 ) ( r − r , ) 0 ...
... magnetic moment can be looked upon as a mark of " compositeness . " Suppose Anm ( F , F1 , ... ... ... , r ^ ) = Ĉ q☺ ( r − r ; ) . j1 m Diagonalization should produce a diagonal matrix of the form : S - 1as = = \ { 3 ) ( r − r , ) 0 ...
Page 8
... magnetic moment , K # 0 . Without going into any details of the calculation let us quote the results . In the case when only one Coulomb potential is present ( hence B = 0 , but E0 ) , we have M ( A ) ~ ix , + + { S db exp ( ia - b ) ...
... magnetic moment , K # 0 . Without going into any details of the calculation let us quote the results . In the case when only one Coulomb potential is present ( hence B = 0 , but E0 ) , we have M ( A ) ~ ix , + + { S db exp ( ia - b ) ...
Page 9
... magnetic moment and define the magnetic moment operator e M = ( 1 + x ) - s , 2m ( 2.6 ) ( S - spin operator ) , where i determines the value of the magnetic moment . When = 0 the equations of motion of such a particle are the so ...
... magnetic moment and define the magnetic moment operator e M = ( 1 + x ) - s , 2m ( 2.6 ) ( S - spin operator ) , where i determines the value of the magnetic moment . When = 0 the equations of motion of such a particle are the so ...
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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