The charge-dependence of nuclear forces

Abstract

1. Introduction. The theory of heavy electrons recently developed by several authors')" may be considered to give a satisfactory account of the empirically known neutron-proton interaction. However, it now seems well established that there exists a proton-proton interaction of comparable magnitude which is not accounted for equally well. Owing to the fact that the emission of a heavy electron involves the change of a neutron into a proton or vice versa, the first approximation of this theory gives only an exchange force between unlike particles, whereas a force between like particles must be due to double transitions and thus only appears in the second approximation. It is true that the expansion in terms of the number of particles emitted is actually so badly convergent that the second order proton-proton force at distances of about 10~1 3 cm. is found to be not essentially smaller than the first order neutron-proton force (see FHK), but nevertheless this does not explain experimental facts, since the calculated second order force is always repulsive.According to the measurements of Tuve, Heydenburg and Hafstadtf the proton-proton force is definitely attractive, and also apparently is very nearly equal to the neutron-proton force in corresponding anti-symmetrical states. The latter fact has served as the basis of the hypothesis that the forces between the elementary nuclear particles are essentially independent of the charges of the particular particles concerned. In the following work we denote this "chargeindependence hypothesis" by the abbreviation CI-hypothesis. According to this view the observed proton-proton interaction should be exactly equal to the corresponding neutron-proton force, and the neutron-neutron force, which cannot be so directly measured, should also be exactly the same. In the theory of binding energies this hypothesis has proved very useful, particularly because it has made it possible to determine the exchange character of nuclear forces practically uniquely.

An Alternative Model for the Duffin–kemmer–petiau Oscillator

“…Let us recall that the Duffin-Kemmer-Petiau equation [18,19,20] describing a free scalar or vector boson of the nonzero mass m can be written as…”

An experimental study of the reaction p+d → ³He+ π° in the δ(1236) resonance region

“…The association of pi-mesons with charge independence was first made (13) by Kemmer in 1938. The two charged pi-mesons have identical mass and the neutral pi-meson is only 3% less massive.…”

Взаимодействие Π-Мезонов С Нуклонами

“…(Следует заметить; что для описания τρΐχ зарядовых состояний π-мезона требуется трёхкомпонентное поле Ф ; , три компоненты которого образуют век-тор в пространстве изотопического спина. Для того чтобы выполня-лось требование зарядовой независимости, используется «симметриче-ская» теория 5 , в которой вектор Ф ; свйртывается с вектором т г "изотопического спина нуклона.) (для PV), полную релятивистскую теорию взаимодействия π-мезона с нуклсном.…”