Abstract

Classical novae are expected to contribute to the 1809-keV Galactic γγ-ray emission by producing its precursor 26^{26}Al, but the yield depends on the thermonuclear rate of the unmeasured 25^{25}Al(p,γp,γ)26^{26}Si reaction. Using the ββ decay of 26^{26}P to populate the key Jπ=3+J^π=3^+ resonance in this reaction, we report the first evidence for the observation of its exit channel via a 1741.6±0.6(stat)±0.3(syst)1741.6 \pm 0.6 (\textrm{stat}) \pm 0.3 (\textrm{syst}) keV primary γγ ray, where the uncertainties are statistical and systematic, respectively. By combining the measured γγ-ray energy and intensity with other experimental data on 26^{26}Si, we find the center-of-mass energy and strength of the resonance to be Er=414.9±0.6(stat)±0.3(syst)±0.6(lit.)E_r = 414.9 \pm 0.6(\textrm{stat}) \pm 0.3 (\textrm{syst}) \pm 0.6(\textrm{lit.}) keV and ωγ=23±6(stat)−10+11(lit.)ωγ= 23 \pm 6 (\textrm{stat})^{+11}_{-10}(\textrm{lit.}) meV, respectively, where the last uncertainties are from adopted literature data. We use hydrodynamic nova simulations to model 26^{26}Al production showing that these measurements effectively eliminate the dominant experimental nuclear-physics uncertainty and we estimate that novae may contribute up to 30% of the Galactic 26^{26}Al.

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