Interactions of High Energy Particles with Nuclei |
From inside the book
Page 21
This means that near to the nuclear boundary sin ( xc ( 6 ) + Ě ( 6 ) ) is large . It is amusing that numerically Im M with proper xc is approximately the same as Re M without xe ! This is true for 208Pb . In general one gets all kinds ...
This means that near to the nuclear boundary sin ( xc ( 6 ) + Ě ( 6 ) ) is large . It is amusing that numerically Im M with proper xc is approximately the same as Re M without xe ! This is true for 208Pb . In general one gets all kinds ...
Page 22
Most experiments ( e.g. , CERN series - compare [ S1 ] ) have poor energy resolution of the incident and outgoing beam ( ~ 50 MeV ) , hence they sum over all nuclear excitations ( without producing mesons , however ) .
Most experiments ( e.g. , CERN series - compare [ S1 ] ) have poor energy resolution of the incident and outgoing beam ( ~ 50 MeV ) , hence they sum over all nuclear excitations ( without producing mesons , however ) .
Page 28
The nucleon and nuclear targets supplement each other because the nuclear medium amplifies the scattering of the produced objects . The model of diffractive processes described below is based on : M. L. Good and W. D. Walker ( 1960 ) ...
The nucleon and nuclear targets supplement each other because the nuclear medium amplifies the scattering of the produced objects . The model of diffractive processes described below is based on : M. L. Good and W. D. Walker ( 1960 ) ...
Page 33
The real and imaginary parts of the elastic Ko and Ko - nuclear amplitudes are sketched below . The uncertainties of our knowledge of these amplitudes are also shown [ 26 ] . Imf ( in fermis ) fron frop -3 for ~ 33.
The real and imaginary parts of the elastic Ko and Ko - nuclear amplitudes are sketched below . The uncertainties of our knowledge of these amplitudes are also shown [ 26 ] . Imf ( in fermis ) fron frop -3 for ~ 33.
Page 34
One gets the following nuclear parameters from the best fits [ 26 ] . Pb Cu R , 6.60 fm ср 0.50 fm 4.23 fm these are well known from 0.57 fm elastic scattering ( 4.86 +0.10 ) fm ( 0.74 +0.03 ) fm Rr ( Cn = Cp ) Cn ( Rn = Rp ) ( 7.29 ...
One gets the following nuclear parameters from the best fits [ 26 ] . Pb Cu R , 6.60 fm ср 0.50 fm 4.23 fm these are well known from 0.57 fm elastic scattering ( 4.86 +0.10 ) fm ( 0.74 +0.03 ) fm Rr ( Cn = Cp ) Cn ( Rn = Rp ) ( 7.29 ...
What people are saying - Write a review
We haven't found any reviews in the usual places.
Common terms and phrases
absorption additivity analysis approximately assume attenuation beam Bureau of Standards charge coherent collision complete components compute consider contribution corrections Coulomb Coulomb interactions coupling cross section db exp depend describe deuteron diffractive production processes discussed effects elastic scattering elastic scattering amplitude equation example excited existence exp ia.b experimental experiments expression fact factor field final formula forward given gives Glauber hadrons Hence high energy limit important incident particle inelastic initial Institute interactions introduce magnetic mass materials measurement momentum transfer multiple scattering National Bureau Note nuclear nuclear targets nuclei nucleon numbers objects obtained parameters phase shifts photon photoproduction physical position possible problem profiles shadowing single Standards step strong structure technical vector meson wave function