A study of the 208Pb(d,p)209Pb reaction at energies above and below the Coulomb barrier

doi:10.1016/0375-9474(69)90988-9

Nuclear Physics A

Volume 128, Issue 1, 28 April 1969, Pages 224-240

https://doi.org/10.1016/0375-9474(69)90988-9 Get rights and content

Abstract

The ²⁰⁸Pb(d,p)²⁰⁹Pb reaction has been studied at deutron bombarding energies of 8, 9, 10, 16.5 and 18.7 MeV.

The single-particle character of the low-lying levels of ²⁰⁹Pb has been exploited to assess the accuracy of the spectroscopic factors obtained from a distorted wave Born approximation analysis of the proton angular distributions.

Various corrections to the standard zero-range calculations are investigated and the special advantages of the experiments performed at energies below the Coulomb barrier are evaluated.

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The experimental data are evaluated for known nuclides of mass number A = 209 (Au,Hg,Tl,Pb,Bi,Po,At,Rn, Fr,Ra,Ac,Th). Detailed evaluated level properties and related nuclear structure information are presented, with the best values recommended for level energies, half-lives, γ–ray energies and intensities, decay data (energies, intensities and placement of radiations), and other spectroscopic data. This work supersedes the earlier full evaluation of A = 209 by M.J. Martin (1991Ma16).
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A study of the nucleus 52Cr using the 51V(τ, d)52Cr reaction at 15 MeV
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Angular distributions of the (τ, d) and (τ, τ) reactions on ⁵¹V have been measured at E_τ = 15 MeV using a multichannel magnetic spectrograph. Optical model parameters have been obtained from an analysis of the elastic scattering. These parameters have been used to calculate theoretical angular distributions using the DWBA. Spectroscopic factors and l_p values for ⁵²Cr levels up to E_x = 8.4 MeV were obtained by comparison of the data with the DWBA theory. Many levels due to l_p = 0, 1, 3 and 1 + 3 transfers not previously seen in proton stripping reactions are reported. The Spectroscopic information obtained is compared with that from other reactions leading to ⁵²Cr. This has enabled tentative suggestions to be made concerning the wave functions of several of the states. A comparison is also made with the available theoretical calculations and it is concluded that further calculations are required using a much larger configuration space and possibly core excitations.
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^†: Present address: Chalk River Nuclear Laboratories, Chalk River, Ontario, Canada.

^††: Present address: Corpus Christi College, Cambridge, England.

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Nuclear Physics A

Abstract

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