학술논문

Backward positive pion production from nuclei bombarded with 600 MeV protons, 700 MeV alpha particles, and 350 MeV deuterons
Document Type
Journal Article
Author
Source
Phys. Rev., C; (United States); 18:4
Subject
73 NUCLEAR PHYSICS AND RADIATION PHYSICS ALPHA REACTIONS
INCLUSIVE INTERACTIONS
CARBON
DEUTERON REACTIONS
PROTON REACTIONS
COBALT
LITHIUM 6 TARGET
PIONS PLUS
PARTICLE PRODUCTION
TANTALUM
ANGULAR DISTRIBUTION
CROSS SECTIONS
MEV RANGE 100-1000
SHELL MODELS
WAVE FUNCTIONS
BARYON REACTIONS
BOSONS
CHARGED-PARTICLE REACTIONS
DISTRIBUTION
ELEMENTARY PARTICLES
ELEMENTS
ENERGY RANGE
FUNCTIONS
HADRON REACTIONS
HADRONS
INTERACTIONS
MATHEMATICAL MODELS
MESONS
METALS
MEV RANGE
NONMETALS
NUCLEAR MODELS
NUCLEAR REACTIONS
NUCLEON REACTIONS
PARTICLE INTERACTIONS
PIONS
PSEUDOSCALAR MESONS
REFRACTORY METALS
TARGETS
TRANSITION ELEMENTS 651325* -- Nuclear Properties & Reactions, A=6-19, Experimental-- Nuclear Reactions & Scattering-- (-1987)
651525 -- Nuclear Properties & Reactions, A=39-58, Experimental-- Nuclear Reactions & Scattering-- (-1987)
651825 -- Nuclear Properties & Reactions, A=150-189, Experimental-- Nuclear Reactions & Scattering-- (-1987)
Language
English
Abstract
The momentum dependence, at fixed pion angles of 180 and 155/sup 0/, of inclusive pion production reactions has been obtained for 600 MeV protons and 175 MeV/nucleon ..cap alpha.. particles and deuterons on /sup 6/Li, C, Co, and Ta. The spectra obtained all fall off exponentially with increasing pion momentum, the slope being about 30 MeV/c independent of either target or projectile nature. The data are examined from the point of view of quasi-two-body scaling, a reaction description discussed recently which suggests that q/sub min/, the minimum nuclear recoil momentum possible kinematically, is the proper scaling variable. When plotted versus q/sub mmin/, all data presented here keep their exponential shape, but the slope becomes 70 MeV/c, i.e., nearly the same as obtained for proton production by the same selection of beam projectiles and energies. It is concluded that the same functional of the target momentum space wave function is revealed by quasi-two-body scaling in inclusive pion production experiments, as in inclusive proton and light-fragment production experiments. Finally, the results of a Monte Carlo calculation of pion spectra based on a single NN ..-->.. ..pi..NN interaction and taking into account the internal motion of the nucleons in target and projectile are presented. The shape and cross sections are accounted for when effective momentum densities of exponential forms are used; the slope constants necessary are compatible with the ones obtained in quasi-two-body scaling. Using thee ground state momentum density of an independent particle shell model produces pion spectra which fall off too rapidly. Furthermore, the Monte Carlo calculation reveals kinematical features of the reaction, which help explain why quasi-two-body scaling works for pion production.