Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |
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... WASHINGTON : 1975 For sale by the Superintendent of Documents , U.S. Government Printing Office Washington , D.C. , 20402 - Price $ 1.35 Stock Number 0303-01317 Preface This monograph is based on lectures given by Dr.
... WASHINGTON : 1975 For sale by the Superintendent of Documents , U.S. Government Printing Office Washington , D.C. , 20402 - Price $ 1.35 Stock Number 0303-01317 Preface This monograph is based on lectures given by Dr.
Page 10
... numbers can be neglected ) . Let us start with just one scatterer : TARGET SHADOW 2 = 0 The incident wave : ekz . The wave immediately behind the scatterer : ≈eikz - y ( b ) eikz , b = ( x , y ) . The shape of the shadow is given by y ...
... numbers can be neglected ) . Let us start with just one scatterer : TARGET SHADOW 2 = 0 The incident wave : ekz . The wave immediately behind the scatterer : ≈eikz - y ( b ) eikz , b = ( x , y ) . The shape of the shadow is given by y ...
Page 12
... numbers + anomalous magnetic moment ) breaks down the " ansatz " of additivity of phase shifts . We can also have a look at this problem from the point of view of a Glauber - like description of scattering of two composite objects . The ...
... numbers + anomalous magnetic moment ) breaks down the " ansatz " of additivity of phase shifts . We can also have a look at this problem from the point of view of a Glauber - like description of scattering of two composite objects . The ...
Page 20
... number of neutrons , Z - number of protons ) : - ixs ( b ) ≈ — Nyn ( 0 ) În ( b ) — ZYp ( 0 ) Pp ( b ) . Pn When yn ( b ) and y , ( b ) are very sharp compared with pn ( s ) and pp ( s ) we have ix . ( b ) ≈ - Nyn ( 0 ) În ( b ) — ZYp ...
... number of neutrons , Z - number of protons ) : - ixs ( b ) ≈ — Nyn ( 0 ) În ( b ) — ZYp ( 0 ) Pp ( b ) . Pn When yn ( b ) and y , ( b ) are very sharp compared with pn ( s ) and pp ( s ) we have ix . ( b ) ≈ - Nyn ( 0 ) În ( b ) — ZYp ...
Page 22
... number of nucleons . Indeed one can show ( compare ref . [ 15 ] -the calculation was done with the Coulomb interactions present ) that to a good approximation ( note that since this formula does not exhibit a forward dip , it is not ...
... number of nucleons . Indeed one can show ( compare ref . [ 15 ] -the calculation was done with the Coulomb interactions present ) that to a good approximation ( note that since this formula does not exhibit a forward dip , it is not ...
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