1955
DOI: 10.1103/physrev.97.1205
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Cross Sections for Nonelastic Interactions of 14-Mev Neutrons with Various Elements

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Cited by 89 publications
(3 citation statements)
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“…The two-component theory requires non-identity of neutrino (helicity -1) and antineutrino (helicity + l ) , where the former is defined as the neutral particle emitted in p' decay and the latter as that emitted in pdecay. Such non-identity was consistent with the enormously long mean life of nuclei undergoing double p decay (see 5 8) and also with the experiment of Davis et a1 (1955) who attempted to observe the reaction…”
supporting
confidence: 80%
“…The two-component theory requires non-identity of neutrino (helicity -1) and antineutrino (helicity + l ) , where the former is defined as the neutral particle emitted in p' decay and the latter as that emitted in pdecay. Such non-identity was consistent with the enormously long mean life of nuclei undergoing double p decay (see 5 8) and also with the experiment of Davis et a1 (1955) who attempted to observe the reaction…”
supporting
confidence: 80%
“…Experimental determinations of the total inelastic scattering cross section have not been reported (an upper limit of 730 260 mb has been given by Graves and Davis [4]). Measurements on the (n,2n) cross section have resulted in different values.…”
Section: Introductionmentioning
confidence: 99%
“…O método consistia em observar a luz de cintilação produzida pelo pósitron da reação de decaimento beta inverso, seguida, alguns microsegundos depois, pelo raio gama da captura do nêutron em um alvo de cádmio. Em um experimento separado, a reação: , não foi observada [14] . Este f ato se dá porque o neutrino e o antineutrino são partículas diferentes ( e e ν ≠ ν…”
Section: X(?)unclassified