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Featured researches published by Lori Downen.


The Astrophysical Journal | 2013

NUCLEAR MIXING METERS FOR CLASSICAL NOVAE

K. J. Kelly; Christian Iliadis; Lori Downen; Jordi Jose; Arthur E. Champagne

Classical novae are caused by mass transfer episodes from a main-sequence star onto a white dwarf via Roche lobe overflow. This material possesses angular momentum and forms an accretion disk around the white dwarf. Ultimately, a fraction of this material spirals in and piles up on the white dwarf surface under electron-degenerate conditions. The subsequently occurring thermonuclear runaway reaches hundreds of megakelvin and explosively ejects matter into the interstellar medium. The exact peak temperature strongly depends on the underlying white dwarf mass, the accreted mass and metallicity, and the initial white dwarf luminosity. Observations of elemental abundance enrichments in these classical nova events imply that the ejected matter consists not only of processed solar material from the main-sequence partner but also of material from the outer layers of the underlying white dwarf. This indicates that white dwarf and accreted matter mix prior to the thermonuclear runaway. The processes by which this mixing occurs require further investigation to be understood. In this work, we analyze elemental abundances ejected from hydrodynamic nova models in search of elemental abundance ratios that are useful indicators of the total amount of mixing. We identify the abundance ratios ΣCNO/H, Ne/H, Mg/H, Al/H, and Si/H as useful mixing meters in ONe novae. The impact of thermonuclear reaction rate uncertainties on the mixing meters is investigated using Monte Carlo post-processing network calculations with temperature-density evolutions of all mass zones computed by the hydrodynamic models. We find that the current uncertainties in the 30P(p, γ)31S rate influence the Si/H abundance ratio, but overall the mixing meters found here are robust against nuclear physics uncertainties. A comparison of our results with observations of ONe novae provides strong constraints for classical nova models.


The Astrophysical Journal | 2018

On presolar stardust grains from CO classical novae

Christian Iliadis; Lori Downen; Jordi Jose; Larry R. Nittler; Sumner G. Starrfield

About 30% to 40% of classical novae produce dust 20-100 days after the outburst, but no presolar stardust grains from classical novae have been unambiguously identified yet. Although several studies claimed a nova paternity for certain grains, the measured and simulated isotopic ratios could only be reconciled assuming that the grains condensed after the nova ejecta mixed with a much larger amount of close-to-solar matter. However, the source and mechanism of this potential post-explosion dilution of the ejecta remains a mystery. A major problem with previous studies is the small number of simulations performed and the implied poor exploration of the large nova parameter space. We report the results of a different strategy, based on a Monte Carlo technique, that involves the random sampling over the most important nova model parameters: the white dwarf composition; the mixing of the outer white dwarf layers with the accreted material before the explosion; the peak temperature and density; the explosion time scales; and the possible dilution of the ejecta after the outburst. We discuss and take into account the systematic uncertainties for both the presolar grain measurements and the simulation results. Only those simulations that are consistent with all measured isotopic ratios of a given grain are accepted for further analysis. We also present the numerical results of the model parameters. We identify 18 presolar grains with measured isotopic signatures consistent with a CO nova origin, without assuming any dilution of the ejecta. Among these, the grains G270 2, M11-334-2, G278, M11-347-4, M11-151-4, and Ag2 6 have the highest probability of a CO nova paternity.


The Astrophysical Journal | 2013

NUCLEAR THERMOMETERS FOR CLASSICAL NOVAE

Lori Downen; Christian Iliadis; Jordi Jose; Sumner G. Starrfield


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2010

Ratio of germanium detector peak efficiencies at photon energies of 4.4 and 11.7 MeV: Experiment versus simulation

Spencer Carson; Christian Iliadis; J. M. Cesaratto; Arthur E. Champagne; Lori Downen; Marija Ivanovic; J. H. Kelley; Richard Longland; J. R. Newton; G. Rusev; A. P. Tonchev


Physical Review C | 2015

High-intensity-beam study of O 17 ( p , γ ) F 18 and thermonuclear reaction rates for O 17 + p

M. Q. Buckner; C. Iliadis; K. J. Kelly; Lori Downen; A. E. Champagne; J. M. Cesaratto; C. Howard; R. Longland


Physical Review C | 2017

New measurements of low-energy resonances in the Ne 22 (p,γ) Na 23 reaction

K. J. Kelly; A. E. Champagne; Lori Downen; J. R. Dermigny; S. Hunt; Christian Iliadis; A. L. Cooper


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2015

Performance of A Compact Multi-crystal High-purity Germanium Detector Array for Measuring Coincident Gamma-ray Emissions

C. Howard; S. Daigle; Matt Buckner; Luke E. Erikson; Robert C. Runkle; Sean C. Stave; Arthur E. Champagne; Andrew I. Cooper; Lori Downen; Brian D. Glasgow; K. J. Kelly; Anne Sallaska


Bulletin of the American Physical Society | 2014

The thermonuclear reaction rate of

Matthew Quinn Buckner; Christian Iliadis; K. J. Kelly; Lori Downen; Arthur E. Champagne; J. M. Cesaratto; Richard Longland


Proceedings of XII International Symposium on Nuclei in the Cosmos — PoS(NIC XII) | 2013

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Lori Downen; Christian Iliadis; Jordi Jose; Sumner G. Starrfield


Unknown Journal | 2012

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Lori Downen; Christian Iliadis; Jordi Jose; Sumner G. Starrfield

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Christian Iliadis

University of North Carolina at Chapel Hill

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K. J. Kelly

University of North Carolina at Chapel Hill

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Jordi Jose

Polytechnic University of Catalonia

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Arthur E. Champagne

University of North Carolina at Chapel Hill

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J. M. Cesaratto

University of North Carolina at Chapel Hill

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A. E. Champagne

Oak Ridge National Laboratory

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C. Howard

University of North Carolina at Chapel Hill

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Richard Longland

University of North Carolina at Chapel Hill

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A. L. Cooper

University of North Carolina at Chapel Hill

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