## Interactions of High Energy Particles with NucleiNational Bureau of Standards, 1975 - 69 pages |

### From inside the book

Results 1-5 of 9

Page 30

...

...

**regeneration**given below is an example where we know n's however ! ) The situation changes when One must , however , keep in mind that in the case when the coefficients di ; are zero or of the same order of magnitude one does predict ... Page 32

...

...

**regenerate**K , mesons because K ° and K ° interact differently with matter , they are absorbed differently . ( e.g. , Ko ...**regeneration**is sketched . ко ко MACROSCOPIC TARGET One can , however , also observe diffractive production of 32. Page 33

...

...

**regeneration**( which comes from a coherent process whose coherence extends over the whole block of matter ) dominates . The amplitude ( neglecting 8 ) is MKL ° → K ‚ ° = 1⁄2 ( Ko | T | Ko ) – 1⁄2 ‹ Ão | T | Ko ) . Hence MÂ ° → K ... Page 34

...

...

**regeneration**than protons . In this case we have not , however , obtained any new information about the elementary processes and the structure of K ̧ ° and K1o . 2. The main feature of the K**regeneration**process seems to be very general ... Page 42

...

...

**regeneration**problem : we are expanding our physical states into states which are " physical in their strong interactions . " Since we know strongly interacting vector mesons with the same quantum numbers as the photon , the simplest ...### 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