| 2025 |
K. Lund, R. Somasundaram, G. C. McLaughlin, J. Miller, et al. |
Kilonova emissions from neutron star merger remnants: implications for nuclear equation of state |
ApJ 987 56 |
|
| 2024 |
D. Ray, N. Vassh, B. Liu, A. A. Valverde, et al. |
Mass measurements of neutron-rich nuclides using the Canadian Penning Trap to inform predictions in the r-process rare-earth peak region |
submitted |
|
| 2024 |
M. Mumpower, T. M. Sprouse, J. Miller, K. Lund, et al. |
Nuclear uncertainties associated with the ejecta of a black-hole accretion disk |
ApJ 970 173 |
|
| 2024 |
K. Lund, G. C. McLaughlin, J. Miller, M. Mumpower |
Magnetic field strength effects on nucleosynthesis from neutron star merger outflows |
ApJ 964 111 |
|
| 2024 |
T. M. Sprouse, K. Lund, J. Miller, G. C. McLaughlin, et al. |
Emergent nucleosynthesis from a 1.2 second long simulation of a black-hole accretion disk |
ApJ 962 79 |
|
| 2024 |
N. Vassh, X. Wang, M. Lariviere, T. M. Sprouse, et al. |
Thallium-208: a beacon of in situ neutron capture nucleosynthesis |
PRL 132 052701 |
|
| 2023 |
E. Holmbeck, J. Barnes, K. Lund, T. M. Sprouse, et al. |
Superheavy elements in kilonovae |
ApJL 951 L13 |
|
| 2023 |
K. Lund, J. Engel, G. C. McLaughlin, M. Mumpower, et al. |
The influence of beta decay rates on r-process observables |
ApJ 944 144 |
|
| 2022 |
N. Vassh, G. C. McLaughlin, M. Mumpower, R. Surman |
Solar data uncertainty impacts on MCMC methods for r-process nucleosynthesis |
Frontiers In Physics |
|
| 2022 |
R. Orford, N. Vassh, J. Clark, G. C. McLaughlin, et al. |
Searching for the origin of the rare-earth peak with precision mass measurements across Ce–Eu isotopic chains |
PRCL 105, 052802 |
|
| 2022 |
N. Vassh, G. C. McLaughlin, M. Mumpower, R. Surman |
The need for a local nuclear physics feature in the neutron-rich rare-earths to explain solar $r$-process abundances |
submitted |
|
| 2021 |
J. Barnes, Y. Zhu, K. Lund, T. M. Sprouse, et al. |
Kilonovae across the nuclear physics landscape: the impact of nuclear physics uncertainties on r-process-powered emission |
ApJ 918 44 |
|
| 2021 |
E. Holmbeck, A. Frebel, G. C. McLaughlin, R. Surman, et al. |
Reconstructing masses of merging neutron stars from stellar r-process abundance signatures |
ApJ 909 21 |
|
| 2021 |
N. Vassh, G. C. McLaughlin, M. Mumpower, R. Surman |
Markov Chain Monte Carlo predictions of neutron-rich lathanide properties as a probe of $r$-process dynamics |
ApJ 907 98 |
|
| 2021 |
Y. Zhu, K. Lund, J. Barnes, T. M. Sprouse, et al. |
Modeling kilonova light curves: dependence on nuclear inputs |
ApJ 906 94 |
|
| 2020 |
N. Vassh, M. Mumpower, G. C. McLaughlin, T. M. Sprouse, et al. |
Co-production of light and heavy $r$-process elements via fission deposition |
ApJ 896 1 |
|
| 2020 |
T. M. Sprouse, R. Navarro Perez, R. Surman, M. Mumpower, et al. |
Propagation of statistical uncertainties of Skyrme mass models to simulations of $r$-process nucleosynthesis |
PRC 101 055803 |
|
| 2019 |
E. Holmbeck, A. Frebel, G. C. McLaughlin, M. Mumpower, et al. |
Actinide-rich and actinide-poor r-process enhanced metal-poor stars do not require separate r-process progenitors |
ApJ 881 1 |
|
| 2019 |
C. Horowitz, A. Arcones, B. Côtè, I. Dillmann, et al. |
r-process nucleosynthesis: connecting rare-isotope beam facilities with the cosmos |
J. Phys. G 46 8 083001 |
|
| 2019 |
N. Vassh, R. Vogt, R. Surman, J. Randrup, et al. |
Using excitation-energy dependent fission yields to identify key fissioning nuclei in r-process nucleosynthesis |
J. Phys. G 46 065202 |
|
| 2018 |
A. Aprahamian, R. Surman, A. Frebel, G. C. McLaughlin, et al. |
FRIB and the GW170817 kilonova |
Whitepaper |
|
| 2018 |
Y. Zhu, R. T. Wollaeger, N. Vassh, R. Surman, et al. |
Californium-254 and kilonova light curves |
ApJL 863 2 |
|
| 2018 |
R. Orford, N. Vassh, J. Clark, G. C. McLaughlin, et al. |
Precision mass measurements of neutron-rich neodymium and samarium isotopes and their role in understanding rare-earth peak formation |
PRL 120, 262702 |
|
| 2017 |
M. Mumpower, G. C. McLaughlin, R. Surman, A. W. Steiner |
Reverse engineering nuclear properties from rare earth abundances in the $r$ process |
J. Phys. G 44 3 034003 |
|
| 2016 |
M. Mumpower, G. C. McLaughlin, R. Surman, A. W. Steiner |
The link between rare earth peak formation and the astrophysical site of the $r$ process |
ApJ 833, 282 |
|
| 2016 |
T. Shafer, J. Engel, C. Fröhlich, G. C. McLaughlin, et al. |
$\beta$ decay of deformed $r$-process nuclei near $A=80$ and $A=160$, including odd-A and odd-odd nuclei, with the Skyrme finite-amplitude method |
PRC 94 055802 |
|
| 2016 |
M. Mumpower, R. Surman, G. C. McLaughlin, A. Aprahamian |
The impact of individual nuclear properties on $r$-process nucleosynthesis |
PPNP 86 86-126 |
|
| 2014 |
R. Surman, M. Mumpower, R. Sinclair, K. Jones, et al. |
Sensitivity studies for a weak $r$ process: neutron capture rates |
AIP Advances 4, 041008 |
|
| 2012 |
M. Mumpower, G. C. McLaughlin, R. Surman |
The influence of neutron capture rates in the rare earth region of the $r$-process abundance pattern |
PRC 86 035803 |
|
| 2012 |
M. Mumpower, G. C. McLaughlin, R. Surman |
The rare earth peak: an overlooked $r$-process diagnostic |
ApJ 752, 117 |
|
| 2012 |
M. Mumpower, G. C. McLaughlin, R. Surman |
Formation of the rare earth peak: gaining insight into late-time $r$-process dynamics |
PRC 85 045801 |
|