A study of the 16O(d, p)17O reaction

Alty, James L.; Green, L.L.; Ruby, R.; Jones, G.D.; Mines, J.R.; Sharpey‐Schafer, J. F.

doi:10.1016/0375-9474(67)90519-2

Cited by 60 publications

(4 citation statements)

References 19 publications

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“…6. The agreement between the theoretical predictions and experimental data [29][30][31] is almost as good as in the case of Fig. 5, the exception being the E d = 12 MeV data from Ref.…”

Section: Resultssupporting

confidence: 73%

“…5, the exception being the E d = 12 MeV data from Ref. [30] whose normalization seems to be inconsistent with the other sets. It is noteworthy that the nonlocal potential NL whose parameters, in contrast to the local potentials CH89 and KD, are independent of the energy, provides a successful description of 16 O(d, p) 17 O and 16 O(d, n) 17 F reactions over a broad range of energies (see Ref.…”

Section: Resultsmentioning

confidence: 83%

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Faddeev-type calculation of(d,n)transfer reactions in three-body nuclear systems

Deltuva

2015

Phys. Rev. C

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Exact Faddeev-type three-body equations are applied to the study of the proton transfer reactions (d, n) in the system consisting of a nuclear core and two nucleons. The integral equations for the three-body transition operators are solved in the momentum-space framework including the Coulomb interaction via the screening and renormalization method. For a weakly bound final nucleus the calculation of the (d, n) reaction is more demanding in terms of the screening radius as compared to the (d, p) reaction. Well converged differential cross section results are obtained for 7 Be(d, n) 8 B, 12 C(d, n) 13 N, and 16 O(d, n) 17 F reactions. A comparison with the corresponding (d, p) reactions is made. The calculations fail to reproduce the shape of the angular distribution for reactions on 12 C but provide quite successful description for reactions on 16 O, especially for the transfer to the 17 F excited state 1/2 + when using a nonlocal optical potential.

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“…6. The agreement between the theoretical predictions and experimental data [29][30][31] is almost as good as in the case of Fig. 5, the exception being the E d = 12 MeV data from Ref.…”

Section: Resultssupporting

confidence: 73%

Section: Resultsmentioning

confidence: 83%

Faddeev-type calculation of(d,n)transfer reactions in three-body nuclear systems

Deltuva

2015

Phys. Rev. C

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“…The data analyzed here include the following adding and removing reactions performed on the same targets: (d,p), (p,d), (α, 3 He), and ( 3 He,α) on 58,60,62,64 Ni [2,3], 74,76 Ge, 76,78 Se [4], and 130 Te [12]. Those data for which just adding or removing reactions were probed include: 16 O(d,p) [13], 40 Ca(d,p) [14], 48 Ca(d,p) [15], the (d,p) and (α, 3 He) reactions on 88 Sr, 90 Zr, and 92 Mo [16], the (d,p), (p,d), ( 3 He,α), and ( 3 He,d) reactions on 98,100 Mo and 100,102 Ru [17], the 112−124 Sn( 3 He,d) and (α,t) reactions [18], the (p,d), ( 3 He,α), and (α, 3 He) reactions on the stable even N = 82 isotones [19,20], and the (d,p) [21] and (α, 3 He) [22] reactions on 208 Pb. In the case where there were no published numerical cross section values, angular-distribution plots were digitized and data extracted, with an increase in the uncertainties from this process estimated as < 5%.…”

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confidence: 99%

Quenching of Cross Sections in Nucleon Transfer Reactions

2013

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Cross sections for proton knockout observed in (e,e'p) reactions are apparently quenched by a factor of ∼0.5, an effect attributed to short-range correlations between nucleons. Here we demonstrate that such quenching is not restricted to proton knockout, but a more general phenomenon associated with any nucleon transfer. Measurements of absolute cross sections on a number of targets between 16O and 208Pb were analyzed in a consistent way, with the cross sections reduced to spectroscopic factors through the distorted-wave Born approximation with global optical potentials. Across the 124 cases analyzed here, induced by various proton- and neutron-transfer reactions and with angular momentum transfer ℓ=0-7, the results are consistent with a quenching factor of 0.55. This is an apparently uniform quenching of single-particle motion in the nuclear medium. The effect is seen not only in (d,p) reactions but also in reactions with A=3 and 4 projectiles, when realistic wave functions are used for the projectiles.

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“…For these analyses, a mix of old and new data were considered. These include: 16 O(d,p) [246], 40 Ca(d,p) [226], 48 Ca(d,p) [247], the (d,p) and (α, 3 He) reactions on 88 Sr, 90 Zr, and [250], the (p,d), ( 3 He,α), and (α, 3 He) reactions on the stable even N = 82 isotones [251,252], and the (d,p) [199] and (α, 3 He) [253] reactions on 208 Pb (this list and further details are available in Ref. [238]).…”

Section: Quenching Of Transfer Reaction Cross Sectionsmentioning

confidence: 99%

Quenching of single-particle strength from direct reactions with stable and rare-isotope beams

Aumann,

Barbieri,

Bazin

et al. 2020

Preprint

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In this review article we discuss the present status of direct nuclear reactions and the nuclear structure aspects one can study with them. We discuss the spectroscopic information we can assess in experiments involving transfer reactions, heavy-ion-induced knockout reactions and quasifree scattering with (p, 2p), (p, pn), and (e, e p) reactions. In particular, we focus on the proton-toneutron asymmetry of the quenching of the spectroscopic strength.

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A study of the 16O(d, p)17O reaction

Cited by 60 publications

References 19 publications

Faddeev-type calculation of(d,n)transfer reactions in three-body nuclear systems

Faddeev-type calculation of(d,n)transfer reactions in three-body nuclear systems

Quenching of Cross Sections in Nucleon Transfer Reactions

Quenching of single-particle strength from direct reactions with stable and rare-isotope beams

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