Low energy scattering cross section ratios of 14N(p, p)14N

Background: The slowest reaction in the first CNO cycle is N-14(p,gamma)O-15, therefore its rate determines the overall energy production efficiency of the entire cycle. The cross section presents several strong resonance contributions, especially for the ground-state transition. Some of the properties of the corresponding levels in the O-15 compound nucleus remain uncertain, which affects the uncertainty in extrapolating the capture cross section to the low energy range of astrophysical interest. Purpose: The N-14(p,gamma) O-15 cross section can be described by using the phenomenological R matrix. Over the energy range of interest, only the proton and gamma-ray channels are open. Since resonance capture makes significant contributions to the N-14(p,gamma) O-15 cross section, resonant proton scattering data can be used to provide additional constraints on the R-matrix fit of the capture data. Methods: A 4 MV KN Van de Graaff accelerator was used to bombard protons onto a windowless gas target containing enriched 14N gas over the proton energy range from E-p = 1.0 to 3.0 MeV. Scattered protons were detected at theta(lab) = 90 degrees, 120 degrees, 135 degrees, 150 degrees, and 160 degrees using ruggedized silicon detectors. In addition, a 10 MV FN Tandem Van de Graaff accelerator was used to accelerate protons onto a solid Adenine (C5H5N5) target, of natural isotopic abundance, evaporated onto a thin self-supporting carbon backing, over the energy range from E-p = 1.8 to 4.0 MeV. Scattered protons were detected at 28 angles between theta(lab) = 30.4 degrees and 167.7 degrees by using silicon photodiode detectors. Results: Relative cross sections were extracted from both measurements. While the relative cross sections do not provide as much constraint as absolute measurements, they greatly reduce the dependence of the data on otherwise significant systematic uncertainties, which are more difficult to quantify. The data are fit simultaneously using an R-matrix analysis and level energies and proton widths are extracted. Even with relative measurements, the statistics and large angular coverage of the measurements result in more confident values for the energies and proton widths of several levels; in particular, the broad resonance at E-c.m. = 2.21 MeV, which corresponds to the 3/2(+) level at E-x = 9.51 MeV in O-15. In particular, the s- and d-wave angular-momentum channels are separated. Conclusion: The relative cross sections provide a consistent set of data that can be used to better constrain a full multichannel R-matrix extrapolation of the capture data. It has been demonstrated how the scattering data reduce the uncertainty through a preliminary Monte Carlo uncertainty analysis, but several other issues remain that make large contributions to the uncertainty, which must be addressed by further capture and lifetime measurements.