Isobaric analogue resonances in 141Pr by elastic and inelastic proton scattering from 140Ce

Marquardt, N.; Rauser, P.; Brentano, P. von; Wurm, J.P.; Zaidi, S. A. A.

doi:10.1016/0375-9474(71)90162-x

Cited by 22 publications

(4 citation statements)

References 22 publications

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“…The formula (13) is identical with the corresponding ones given in [10] and [11] but does not lead to (3.11) from [9] although it was derived under the same assumptions.…”

Section: (8)mentioning

confidence: 89%

“…The sum in (8) runs over all resonances in the studied energy interval, thus replacing the double sum in (5 In obtaining (12), the spin-flip potential scattering described by pO was assumed to be negligible [9,10,11]. The formula (13) is identical with the corresponding ones given in [10] and [11] but does not lead to (3.11) from [9] although it was derived under the same assumptions.…”

Section: (8)mentioning

confidence: 97%

“…A Taylor expansion of the parameters around some energy near the observed resonance gives, after retaining the first two terms, the following expression [9]:…”

Section: Do -Ia(e O)[2 +Ib(e O)lmentioning

confidence: 99%

“…As it can be seen below, the assignment l= 2 for this resonance is consistent with the angular correlation data too. Whenever it was possible, a first guess of the resonance energies and their total and partial widths was done based on a geometrical method ( [9] and references therein). A word of care is still necessary about the J assignments when l# 0 and angular correlations data are missing.…”

Section: Ep (Me V/mentioning

confidence: 99%

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Study of isobaric analogue resonances in65Cu by proton scattering from64Ni

Berinde¹,

Vlăducă²,

Zoran³

et al. 1978

Z Physik A

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Excitation functions of the elastic proton scattering by 64Ni were measured in the energy range Ep = 5.0-6.2 MeV at 90 ~ 125 ~ and 141 ~ and in the energy intervals 5.00-5.25 MeV at 110 ~ and 160 ~ At 90 ~ the excitation function of the inelastic proton scattering leading to the 2 + (1.34 MeV) state in 64Ni was measured too. Out of tile ten resonances found in the whole energy range, the resonances at 5.105, 5.985, 6.042 and 5.35 MeV were studied in more detail. The analysis of the elastic scattering provided the energy, orbital momentum, total and partial widths of the first three resonances. The inelastic scattering cross section for the last three resonances was sufficient to permit the spin determination by (p, P'7) angular correlations in the Goldfarb-Seyler geometry. The spectroscopic factors Spp are in good agreement with those obtained from (d, p) experiments. The resonance at 5.35 MeV exhibits an important 2p @2 + amplitude in its wave function. Its inelastic partial widths and the corresponding spectroscopic factors Spp, were determined. The nonresonant background in the elastic channel is well described by shape and compound elastic scattering calculations with Percy's optical model parameters.

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“…The formula (13) is identical with the corresponding ones given in [10] and [11] but does not lead to (3.11) from [9] although it was derived under the same assumptions.…”

Section: (8)mentioning

confidence: 89%

Section: (8)mentioning

confidence: 97%

“…A Taylor expansion of the parameters around some energy near the observed resonance gives, after retaining the first two terms, the following expression [9]:…”

Section: Do -Ia(e O)[2 +Ib(e O)lmentioning

confidence: 99%

Section: Ep (Me V/mentioning

confidence: 99%

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