By A. B. Kurepin (auth.), Academician D. V. Skobel’tsyn (eds.)
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Extra resources for Studies of Nuclear Reactions
RV § 2. Yp the minimum possible y2 for given values of 'Y~· A similar construction can be obtained for other radii. It then turns out that with increasing interaction range, the shaded region shifts toward higher y~/ 'Y~· Therefore, in order to achieve agreement with the experimental variation of the phase, the widths can only be taken equal for radii a > 4 f.
An analysis of p-T scattering measurements at energies above 1 MeV was performed in an earlier paper  without taking into account reactions and spin-orbital splitting. Eight solutions were obtained, but none of the phases exhibited a clearly defined resonance character. Balashko et al.  have performed measurements on p-T scattering at energies below 200 keV and have carried out the corresponding phase analysis. They found that the contribution due to p phases at these energies did not exceed 1 o/o (at 2l)O keV and 9 = 120•).
They found that the contribution due to p phases at these energies did not exceed 1 o/o (at 2l)O keV and 9 = 120•). Interference with Coulomb scattering facilitated the phase PROTON-TRITIUM REACTIONS BELOW (p,n) REACTION THRESHOLD 27 analysis. However, two solutions were obtained and there was no way of establishing which of these was correct. 7 keY II 36, = 60 ± so 36o = - s· ± t 0 360 = 30 ± 30 360 = - zo ± zo 16o=-15o±7o 16o =- So±go t6o = T ±so, Ep 118 keY = I 16o = 17o ± 12o II where 1&0 is the singlets phase, and 36 0 is the triplets phase.