1983
DOI: 10.1016/0375-9474(83)90085-4
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The analyzing power for the 2H(d, n)3Heg.s. reaction from 5.5 to 11.5 MeV

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Cited by 6 publications
(6 citation statements)
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“…The data are from Refs. [40] (+), [45] (2), [46] (×), [47] ( ), [48] (•), [49] (•), and [23] ( ). ate disagreements, mostly in the vector observables: the minima of iT 11 are underpredicted while the positive peak of P y is shifted to larger angles.…”
Section: Tablementioning
confidence: 99%
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“…The data are from Refs. [40] (+), [45] (2), [46] (×), [47] ( ), [48] (•), [49] (•), and [23] ( ). ate disagreements, mostly in the vector observables: the minima of iT 11 are underpredicted while the positive peak of P y is shifted to larger angles.…”
Section: Tablementioning
confidence: 99%
“…For most observables several measurements exist [40,[45][46][47][48][49]23] that are at variance in particular cases, especially for iT 11 . Nevertheless, the overall description of the experimental data by our calculations is successful with only few small or at most moder- Fig.…”
Section: Tablementioning
confidence: 99%
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“…However, there are also a few disagreements with the data whose magnitude is sensitive to the force model used and may serve as a fertile ground for the investigation of nuclear interactions. Still missing in this study is the extension of the nucleon transfer reactions 2 H(d, p) 3 H and 2 H(d, n) 3 He initiated by deuteron-deuteron collisions at energies well above the breakup threshold where the existing differential cross section and analyzing power data [20][21][22][23][24][25][26][27][28][29][30][31][32] show a complicated structure involving several maxima and minima that change with the energy. Therefore in * arnoldas.deltuva@tfai.vu.lt the present manuscript we aim to investigate 2 H(d, p) 3 H and 2 H(d, n) 3 He reactions up to about 25 MeV deuteron beam energy.…”
Section: Introductionmentioning
confidence: 99%