The uncertainty on the Argonne neutrino spectrum shown in Fig. 27(c) is incorrect. Here, we bring the same figure with the correct uncertainty as given in Ref. [19]. We note that this uncertainty includes the theoretical uncertainty from the recoil-order corrections which is roughly half as large as the uncertainty from the α-spectrum measurement [19]. The conclusions of the paper are unaffected. FIG. 27. (Color online) (a) Neutrino spectrum calculated using the E x distribution obtained in the present study neglecting recoil terms and radiative corrections. Note that the end point of the neutrino spectrum (16.96 MeV) is slightly outside the energy range chosen for the plot due to insufficient numerical precision above 16 MeV. (b) 1σ statistical and systematic uncertainties on the present neutrino spectrum. (c) Relative deviation with respect to the neutrino spectrum calculated using the Argonne E x distribution.
No abstract
The most intense gamma-ray line observable from novae is likely to be from positron annihilation associated with the decay of 18 F. The uncertainty in the destruction rate of this nucleus through the 18 F(p,α) 15 O reaction presents a limit to interpretation of any future observed gamma-ray flux. Direct measurements of the cross section of both this reaction and the 18 F(p,p) 18 F reaction have been performed between center of mass energies of 0.5 and 1.9 MeV. Simultaneous fits to both data sets with the R-Matrix formalism reveal several resonances, with the inferred parameters of populated states in 19 Ne in general agreement with previous measurements. Of particular interest, extra strength has been observed above ECM ∼1.3 MeV in the 18 F(p,p) 18 F reaction and between 1.3-1.7 MeV in the 18 F(p,α) 15 O reaction. This is well described by a broad 1/2 + state, consistent with both a recent theoretical prediction and an inelastic scattering measurement. The astrophysical implications of a broad sub-threshold partner to this state are discussed.
Background: Classical novae result from thermonuclear explosions producing several γ-ray emitters which are prime targets for satellites observing in the MeV range. The early ≤ 511 keV gamma-ray emission depends critically on the 18 F(p,α) 15 O reaction rate which, despite many experimental and theoretical efforts, still remains uncertain.Purpose: One of the main uncertainties in the 18 F(p,α) 15 O reaction rate is the contribution in the Gamow window of interference between sub-threshold 19 Ne states and known broad states at higher energies. Therefore the goal of this work is to clarify the existence and the nature of these sub-threshold states.Method: States in the 19 Ne compound nucleus were studied at the Tandem-ALTO facility using the 19 F( 3 He,t) 19 Ne charge exchange reaction. Tritons were detected with an Enge Split-pole spectrometer while decaying protons or α-particles from unbound 19 Ne states were collected, in coincidence, with a double-sided silicon strip detector array. Angular correlations were extracted and constraints on the spin and parity of decaying states established. Results:The coincidence yield at Ex = 6.29 MeV was observed to be high spin, supporting the conclusion that it is indeed a doublet consisting of high spin and low spin components. Evidence for a broad, low spin state was observed around 6 MeV. Branching ratios were extracted for several states above the proton threshold and were found to be consistent with the literature. R-matrix calculations show the relative contribution of sub-threshold states to the astrophysically important energy region above the proton threshold. Conclusions:The levels schemes of 19 Ne and 19 F are still not sufficiently well known and further studies of the analogue assignments are needed. The tentative broad state at 6 MeV may only play a role if the reduced proton width is large.
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