J-type Carbon Stars: A Dominant Source of 14N-rich Presolar SiC Grains of Type AB

Nan Liu1, Thomas Stephan2,3, Patrick Boehnke2,3, Larry R. Nittler1, Conel M. O’D. Alexander1, Jianhua Wang1, Andrew M. Davis2,3,4, Reto Trappitsch2,3,5, and Michael J. Pellin2,3,4,6
The Astrophysical Journal Letters 844 L12 Link to Article [https://doi.org/10.3847/2041-8213/aa7d4c]
1Department of Terrestrial Magnetism, Carnegie Institution for Science, Washington, DC 20015, USA
2Department of the Geophysical Sciences, The University of Chicago, Chicago, IL 60637, USA
3Chicago Center for Cosmochemistry, Chicago, IL, USA
4The Enrico Fermi Institute, The University of Chicago, Chicago, IL 60637, USA
5Nuclear and Chemical Sciences Division, Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
6Materials Science Division, Argonne National Laboratory, Argonne, IL 60439, USA

We report Mo isotopic data of 27 new presolar SiC grains, including 12 14N-rich AB (14N/15N > 440, AB2) and 15 mainstream (MS) grains, and their correlated Sr and Ba isotope ratios when available. Direct comparison of the data for the MS grains, which came from low-mass asymptotic giant branch (AGB) stars with large s-process isotope enhancements, with the AB2 grain data demonstrates that AB2 grains show near-solar isotopic compositions and lack s-process enhancements. The near-normal Sr, Mo, and Ba isotopic compositions of AB2 grains clearly exclude born-again AGB stars, where the intermediate neutron-capture process (i-process) takes place, as their stellar source. On the other hand, low-mass CO novae and early R- and J-type carbon stars show 13C and 14N excesses but no s-process enhancements and are thus potential stellar sources of AB2 grains. Because both early R-type carbon stars and CO novae are rare objects, the abundant J-type carbon stars (10%–15% of all carbon stars) are thus likely to be a dominant source of AB2 grains.

Reducing Uncertainties in the Production of the Gamma-emitting Nuclei 26Al, 44Ti, and 60Fe in Core-collapse Supernovae by Using Effective Helium Burning Rates

Sam M. Austin1,2, Christopher West2,3,4, and Alexander Heger2,3,5,6
The Astrophysical Journal Letters 839 L9 Link to Article [https://doi.org/10.3847/2041-8213/aa68e7]
1National Superconducting Cyclotron Laboratory, Michigan State University, 640 South Shaw Lane, East Lansing, MI 48824-1321, USA
2Joint Institute for Nuclear Astrophysics—Center for the Evolution of the Elements, Michigan State University, East Lansing, MI 48824-1321, USA
3Minnesota Institute for Astronomy, School of Physics and Astronomy, University of Minnesota, Twin Cities, Minneapolis, MN 55455-0149, USA
4Center for Academic Excellence, Metropolitan State University, St. Paul, MN, 55106, USA
5Monash Centre for Astrophysics, School of Physics and Astronomy, Monash University, VIC 3800, Australia
6Center for Nuclear Astrophysics, Department of Physics and Astronomy, Shanghai Jiao-Tong University, Shanghai 200240, P. R. China

We have used effective reaction rates (ERRs) for the helium burning reactions to predict the yield of the gamma-emitting nuclei 26Al, 44Ti, and 60Fe in core-collapse supernovae (SNe). The variations in the predicted yields for values of the reaction rates allowed by the ERR are much smaller than obtained previously, and smaller than other uncertainties. A “filter” for SN nucleosynthesis yields based on pre-SN structure was used to estimate the effect of failed SNe on the initial mass function averaged yields; this substantially reduced the yields of all these isotopes, but the predicted yield ratio 60Fe/26Al was little affected. The robustness of this ratio is promising for comparison with data, but it is larger than observed in nature; possible causes for this discrepancy are discussed.

Origin and Evolution of Short-period Comets

David Nesvorný1, David Vokrouhlický2, Luke Dones1, Harold F. Levison1, Nathan Kaib3, and Alessandro Morbidelli4
Astrophysical Journal 843, 120 Link to Article [https://doi.org/10.3847/1538-4357/aa7cf6]
1Department of Space Studies, Southwest Research Institute, 1050 Walnut St., Suite 300, Boulder, CO 80302, USA
2Institute of Astronomy, Charles University, V Holešovičkách 2, CZ-18000 Prague 8, Czech Republic
3H.L. Dodge Department of Physics and Astronomy, University of Oklahoma, Norman, OK 73019, USA
4Département Cassiopée, University of Nice, CNRS, Observatoire de la Côte d’Azur, Nice, F-06304, France

Comets are icy objects that orbitally evolve from the trans-Neptunian region into the inner solar system, where they are heated by solar radiation and become active due to the sublimation of water ice. Here we perform simulations in which cometary reservoirs are formed in the early solar system and evolved over 4.5 Gyr. The gravitational effects of Planet 9 (P9) are included in some simulations. Different models are considered for comets to be active, including a simple assumption that comets remain active for ${N}_{{\rm{p}}}(q)$ perihelion passages with perihelion distance $q\lt 2.5\,\mathrm{au}$. The orbital distribution and number of active comets produced in our model is compared to observations. The orbital distribution of ecliptic comets (ECs) is well reproduced in models with ${N}_{{\rm{p}}}(2.5)\simeq 500$ and without P9. With P9, the inclination distribution of model ECs is wider than the observed one. We find that the known Halley-type comets (HTCs) have a nearly isotropic inclination distribution. The HTCs appear to be an extension of the population of returning Oort-cloud comets (OCCs) to shorter orbital periods. The inclination distribution of model HTCs becomes broader with increasing ${N}_{{\rm{p}}}$, but the existing data are not good enough to constrain ${N}_{{\rm{p}}}$ from orbital fits. ${N}_{{\rm{p}}}(2.5)\gt 1000$ is required to obtain a steady-state population of large active HTCs that is consistent with observations. To fit the ratio of the returning-to-new OCCs, by contrast, our model implies that ${N}_{{\rm{p}}}(2.5)\lesssim 10$, possibly because the detected long-period comets are smaller and much easier to disrupt than observed HTCs.