Level structure of 51Cr from the (d, p) reaction on 50Cr

Chowdhury, Shahariar; Majumder, A.R.; Gupta, H. M. Sen

doi:10.1016/0375-9474(77)90173-7

Cited by 17 publications

(15 citation statements)

References 36 publications

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“…The latter is yet increasing slowly with energy up to ∼25 MeV, but then decreases too. However, the measured BU proton-emission cross sections σ p BU at 15 [6], 25.5 [3,6], and 56 MeV [5], and [26][27][28][29][30][31][32][33][34] and calculated elastic-scattering angular distributions of deuterons on 50,52,53,54 Cr at energies from ∼5 to ∼34 MeV, using the global OMP of Daehnick et al [35], and (bottom) measured [34,36] and similarly calculated total-reaction cross sections for deuterons on 52,53,54 Cr from 3 to 60 MeV. the parametrization predictions pointed out the increase of σ p BU with the target-nucleus mass, from 27 Al up to 232 Th, as well as with increasing incident energy (e.g., Fig.…”

Section: B Deuteron Breakupmentioning

confidence: 99%

“…(Bottom) The fractions of σR corresponding to the contributions of BU (dashed curves), DR (solid curves), DI (dash-dotted curves), and PE+CN (dash-dot-dotted curves) mechanisms involved in the d+ 54 Cr interactions (see text).jor role of the stripping (d, n) and (d, p) reactions to the activation cross sections of54 Mn,51 Mn, and 51 Cr residual nuclei, for deuteron interaction with the natural Cr target, is particularly apparent in Figs. 9 and 11, respec-(Color online) Comparison of measured (solid circles)[50] and calculated (solid curves) proton angular distributions of 50 Cr(d, p)51 Cr stripping transitions to states with excitation energies in MeV, at the incident energy of 12 MeV.…”

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confidence: 99%

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Consistent account of deuteron-induced reactions on natCr up to 60 MeV

et al. 2018

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sive BU and DR cross sections is still investigated numerically (e.g., [2] and Refs. therein). On the other hand, the sparce deuteron-breakup experimental data systematics [3][4][5][6][7] related to the high complexity of the breakup mechanism has constrained so far a comprehensive analysis of the deuteron interactions within wide ranges of target nuclei and incident energies. Thus, reaction cross sections recommended most recently for high-priority elements are still based on data fit, e.g. by various-order Pade approximations [8], with so low predictive power and apart from nuclear modeling advance.Consequently, complementary measurements and model calculations are necessary in order to meet the demands of several on-going strategic research programmes of international large-scale facilities [9-11] and databases [12]. The present work aims both to enhance the database of deuteron-induced reactions on natural chromium, up to 20 MeV, and continue a series of recent analyzes [13][14][15][16][17][18] looking for the consistent inclusion of the deuteron BU contribution within activation cross-section account. The experimental setup as well the new mea-

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Section: B Deuteron Breakupmentioning

confidence: 99%

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confidence: 99%

Consistent account of deuteron-induced reactions on natCr up to 60 MeV

et al. 2018

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“…[30]. The spectroscopic factor values of C 2 Sp are the averaged ones from the previous (d,p) experiments [31][32][33], except the assumed value of 0.001. …”

Section: Rate Based On Shell Modelmentioning

confidence: 99%

“…Here, we assumed the proton spectroscopic factor in 51 Co equal to the neutron spectroscopic factor in the 51 Cr mirror, i.e., C 2 S p = C 2 S n . The experimental neutron spectroscopic factors are adopted from the previous (d,p) transfer reactions [31][32][33]. Here, the spectroscopic factor is a model-dependent quantity (see e.g., Ref.…”

Section: Rate Based On Shell Modelmentioning

confidence: 99%