Interactions of High Energy Particles with Nuclei |
From inside the book
Results 1-5 of 19
Page 1
Special attention is paid to the interaction of high energy hadrons and photons . Interactions of high energy electrons and neutrinos are briefly mentioned . The common features of all these processes are emphasized throughout the ...
Special attention is paid to the interaction of high energy hadrons and photons . Interactions of high energy electrons and neutrinos are briefly mentioned . The common features of all these processes are emphasized throughout the ...
Page 2
( Nonetheless there exists a motivation for belief in their existence : as in the case of photons interacting with nucleons — where the strongly interacting vector mesons seem to dominate - in the case of neutrino interactions — as was ...
( Nonetheless there exists a motivation for belief in their existence : as in the case of photons interacting with nucleons — where the strongly interacting vector mesons seem to dominate - in the case of neutrino interactions — as was ...
Page 27
... s ) is constructed from DELBRUCK SCATTERING ELECTRON PHOTON PHOTON POSITRON INITIAL ELECTRON - POSITRON WAVE FUNCTION FINAL ELECTRON - POSITRON Dittractive | WAVE FUNCTION Scattering from the target 1 the " relativistic wave ...
... s ) is constructed from DELBRUCK SCATTERING ELECTRON PHOTON PHOTON POSITRON INITIAL ELECTRON - POSITRON WAVE FUNCTION FINAL ELECTRON - POSITRON Dittractive | WAVE FUNCTION Scattering from the target 1 the " relativistic wave ...
Page 30
First we introduce the physical states of the system , I fi ) ( which are analogous to the states yn and ynxe , of the photon ) . We want to compute ( il T | li ) . We expand Ni ) into a set of states | 1 ; ) whose scattering and ...
First we introduce the physical states of the system , I fi ) ( which are analogous to the states yn and ynxe , of the photon ) . We want to compute ( il T | li ) . We expand Ni ) into a set of states | 1 ; ) whose scattering and ...
Page 41
... established fact that , at high energy , photons exhibit shadowing . The total photo cross sections for complex nuclei vary approximately as A0.9 in the few GeV energy range . It is very suggestive then to accept that photons have 41.
... established fact that , at high energy , photons exhibit shadowing . The total photo cross sections for complex nuclei vary approximately as A0.9 in the few GeV energy range . It is very suggestive then to accept that photons have 41.
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 ground hadrons Hence high energy limit important incident particle inelastic initial Institute interactions introduce magnetic mass measurement momentum transfer multiple scattering National Bureau Note nuclear nuclear targets nuclei nucleon numbers objects obtained parameters phase shifts photon photoproduction physical position possible present problem profiles regeneration shadowing single Standards step strong structure technical vector meson wave function
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 |
| Export Citation | BiBTeX EndNote RefMan |