Classical novae are the results of surface thermonuclear explosions of hydrogen accreted by white dwarfs (WDs) from their low-mass main-sequence or redgiant binary companions. Chemical composition analysis of their ejecta shows that nova outbursts occur on both carbon-oxygen (CO) and more massive oxygen-neon (ONe) WDs, and that there is cross-boundary mixing between the accreted envelope and underlying WD. We demonstrate that the state-of-the-art stellar evolution code MESA and post-processing nucleosynthesis tools of NuGrid can successfully be used for modeling of CO and ONe nova outbursts and nucleosynthesis. The convective boundary mixing (CBM) in our 1D numerical simulations is implemented using a diffusion coefficient that is exponentially decreasing with a distance below the bottom of the convective envelope. We show that this prescription produces maximum temperature evolution profiles and nucleosynthesis yields in good agreement with those obtained using the commonly adopted 1D nova model in which the CBM is mimicked by assuming that the accreted envelope has been pre-mixed with WD's material. In a previous paper, we have found that 3 He can be produced in situ in solar-composition envelopes accreted with slow rates (Ṁ < 10 −10 M ⊙ /yr) by cold (T WD < 10 7 K) CO WDs, and that convection is triggered by 3 He burning before the nova outburst in this case. Here, we confirm this result for ONe novae. Additionally, we find that the interplay between the 3 He production and destruction in the solar-composition envelope accreted with an intermediate rate, e.g.Ṁ = 10 −10 M ⊙ /yr, by the 1.15 M ⊙ ONe WD with a relatively high initial central temperature, e.g. T WD = 15 ×10 6 K, leads to the formation of a thick radiative buffer zone that separates the bottom of the convective envelope from the WD surface.
Excited states in 192 Pt and 194 Pt have been studied with high-energy resolution, in the (p, t) reaction, by using the Q3D magnetic spectrograph at the Munich MP tandem accelerator. Outgoing tritons were recorded at laboratory angles sensitive to the unique shape of the L = 0 angular distribution. Sets of previously unknown 0 + states were identified up to an energy of ∼3 MeV. The 0 + states in 192,194 Pt are discussed in the context of the evolution of intruder states and shape coexistence in the light Pt isotopes.
The17 O(p,γ) 18 F reaction plays a important role in hydrogen burning nucleosynthesis. Conflicting values for the low-energy behavior of its cross section exist in the literature. We present direct measurements of the astrophysical S factor of the 17 O(p,γ) 18 F reaction at center-of-mass energies between 250 and 500 keV. These measurements were conducted in inverse kinematics at the DRAGON recoil separator. 26.50.+x,98.80.Ft,24.50.+g,25.40.Lw
The total cross section of the 12 C+ 16 O fusion reaction has been measured at low energies to investigate the role of this reaction during late stellar evolution burning phases. A high-intensity oxygen beam, produced by the 5MV pelletron accelerator at the University of Notre Dame, impinged on a thick, ultra-pure graphite target. Protons and γ-rays were simultaneously measured in the center-of-mass energy range from 3.64 to 5.01 MeV for singles and from 3.73 to 4.84 MeV for coincidence events, using silicon and Ge detectors. Statistical model calculations were employed to interpret the experimental results. The emergence of a new resonance like broad structure and a decreasing trend in the S-factor data towards lower energies (opposite to previous data) are found for the 12 C+ 16 O fusion reaction. Based on these results the uncertainty range of the reaction rate within the temperature range of late stellar burning environments is being discussed .
Background: Discrepancies exist between the observed abundances of argon and calcium in oxygen-neon nova ejecta and those predicted by nova models. An improved characterization of the 38 K(p, γ) 39 Ca reaction rate over the nova temperature regime (∼ 0.1-0.4 GK), and thus the nuclear structure of 39 Ca above the proton threshold (5770.92(63) keV), is necessary to resolve these contradictions. Purpose: The present study was performed to search for low-spin proton resonances in the 38 K + p system, and to improve the uncertainties in energies of the known astrophysically significant proton resonances in 39 Ca. Method: The level structure of 39 Ca was investigated via high-resolution charged-particle spectroscopy with an Enge split-pole spectrograph using the 40 Ca(3 He, α) 39 Ca reaction. Differential cross sections were measured over 6 laboratory angles at 21 MeV. Distorted-wave Born approximation calculations were performed to constrain the spin-parity assignments of observed levels with special attention to those significant in determination of the 38 K(p, γ) 39 Ca reaction rate over the nova temperature regime. Results: The resonance energies corresponding to two out of three astrophysically important states at 6154(5) and 6472.2(24) keV are measured with better precision than previous charged-particle spectroscopy measurements. A tentatively new state is discovered at 5908(3) keV. The spinparity assignments of a few of the astrophysically important resonances are determined. Conclusions: The present 38 K(p, γ) 39 Ca upper limit thermonuclear reaction rate at 0.1-0.4 GK is higher than that determined in [Physical Review C 97 (2018) 025802] by at most a factor of 1.4 at 0.1 GK.
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