Title: Measuring the 15 O(α, γ) 19 Ne reaction in Type I X-ray bursts using the GADGET II TPC: Hardware
Sensitivity studies have shown that the 15 O(α, γ) 19 Ne reaction is the most important reaction rate uncertainty affecting the shape of light curves from Type I X-ray bursts. This reaction is dominated by the 4.03 MeV resonance in 19 Ne. Previous measurements by our group have shown that this state is populated in the decay sequence of 20 Mg. A single 20 Mg(βp α) 15 O event through the key 15 O(α, γ) 19 Ne resonance yields a characteristic signature: the emission of a proton and alpha particle. To achieve the granularity necessary for the identification of this signature, we have upgraded the Proton Detector of the Gaseous Detector with Germanium Tagging (GADGET) into a time projection chamber to form the GADGET II detection system. GADGET II has been fully constructed, and is entering the testing phase. more »« less
15 O( α , γ ) 19 Ne is regarded as one of the most important thermonuclear reactions in type I X-ray bursts. For studying the properties of the key resonance in this reaction using β decay, the existing Proton Detector component of the Gaseous Detector with Germanium Tagging (GADGET) assembly is being upgraded to operate as a time projection chamber (TPC) at FRIB. This upgrade includes the associated hardware as well as software and this paper mainly focusses on the software upgrade. The full detector set up is simulated using the ATTPCROOTv 2 data analysis framework for 20 Mg and 241 Am.
Wiescher, M.; deBoer, R. J.; Görres, J.
(, The European Physical Journal A)
Abstract The interplay and correlation between the $$^{22}$$ 22 Ne $$(\alpha ,\gamma )^{26}$$ ( α , γ ) 26 Mg and the competing $$^{22}$$ 22 Ne $$(\alpha ,n)^{25}$$ ( α , n ) 25 Mg reaction plays an important role for the interpretation of the $$^{22}$$ 22 Ne $$(\alpha ,n)^{25}$$ ( α , n ) 25 Mg reaction as a neutron source in the s - and n -processes. This paper provides a summary and new data on the $$\alpha $$ α -cluster and single-particle structure of the compound nucleus $$^{26}$$ 26 Mg and the impact on the reaction rate of these two competing processes in stellar helium burning environments.
Chidester, Morgan T; Timmes, F X; Farag, Ebraheem
(, The Astrophysical Journal)
Abstract We consider the combined effects that overshooting and the12C(α,γ)16O reaction rate have on variable white dwarf (WD) stellar models. We find that carbon–oxygen (CO) WD models continue to yield pulsation signatures of the current experimental12C(α,γ)16O reaction rate probability distribution function when overshooting is included in the evolution. These signatures hold because the resonating mantle region, encompassing ≃0.2M⊙in a typical ≃0.6M⊙WD model, still undergoes radiative helium burning during the evolution to a WD. Our specific models show two potential low-order adiabatic g-modes,g2andg6, that signalize the12C(α,γ)16O reaction rate probability distribution function. Both g-mode signatures induce average relative period shifts of ΔP/P= 0.44% and ΔP/P= 1.33% forg2andg6, respectively. We find thatg6is a trapped mode, and theg2period signature is inversely proportional to the12C(α,γ)16O reaction rate. Theg6period signature generally separates the slower and faster reaction rates, and has a maximum relative period shift of ΔP/P= 3.45%. We conclude that low-order g-mode periods from CO WDs may still serve as viable probes for the12C(α,γ)16O reaction rate probability distribution function when overshooting is included in the evolution.
Lam, Yi Hua; Liu, Zi Xin; Heger, Alexander; Lu, Ning; Jacobs, Adam Michael; Johnston, Zac
(, The Astrophysical Journal)
Abstract We reassess the 65 As(p, γ ) 66 Se reaction rates based on a set of proton thresholds of 66 Se, S p ( 66 Se), estimated from the experimental mirror nuclear masses, theoretical mirror displacement energies, and full p f -model space shell-model calculation. The self-consistent relativistic Hartree–Bogoliubov theory is employed to obtain the mirror displacement energies with much reduced uncertainty, and thus reducing the proton-threshold uncertainty up to 161 keV compared to the AME2020 evaluation. Using the simulation instantiated by the one-dimensional multi-zone hydrodynamic code, K epler , which closely reproduces the observed GS 1826−24 clocked bursts, the present forward and reverse 65 As(p, γ ) 66 Se reaction rates based on a selected S p ( 66 Se) = 2.469 ± 0.054 MeV, and the latest 22 Mg( α ,p) 25 Al, 56 Ni(p, γ ) 57 Cu, 57 Cu(p, γ ) 58 Zn, 55 Ni(p, γ ) 56 Cu, and 64 Ge(p, γ ) 65 As reaction rates, we find that though the GeAs cycles are weakly established in the rapid-proton capture process path, the 65 As(p, γ ) 66 Se reaction still strongly characterizes the burst tail end due to the two-proton sequential capture on 64 Ge, not found by the Cyburt et al. sensitivity study. The 65 As(p, γ ) 66 Se reaction influences the abundances of nuclei A = 64, 68, 72, 76, and 80 up to a factor of 1.4. The new S p ( 66 Se) and the inclusion of the updated 22 Mg( α ,p) 25 Al reaction rate increases the production of 12 C up to a factor of 4.5, which is not observable and could be the main fuel for a superburst. The enhancement of the 12 C mass fraction alleviates the discrepancy in explaining the origin of the superburst. The waiting point status of and two-proton sequential capture on 64 Ge, the weak-cycle feature of GeAs at a region heavier than 64 Ge, and the impact of other possible S p ( 66 Se) are also discussed.
Boomershine, C N; Bardayan, D W; Carmichael, S; Caves, L; Davis, A; deBoer, R J; Gula, A; Howard, K; Kelmar, R; Mitchell, A; et al
(, Journal of Physics: Conference Series)
Abstract The20Ne(α,p)23Na reaction rate is important in determining the final abundances of various nuclei produced in type Ia supernovae. Previously, the ground state cross section was calculated from time reversal reaction experiments using detailed balance. The reaction rates extracted from these studies do not consider contributions from the population of excited states, and therefore, are only estimates. A resonance scan, populating both the ground and first excited states, was performed for the20Ne(α,p)23Na reaction, measuring between 2.9 and 5 MeV center of mass energies at the Nuclear Science Lab at the University of Notre Dame. Data analysis is underway and preliminary results show substantial contribution from the excited state reaction.
Wheeler, Tyler, Adams, A., Allmond, J., Alvarez Pol, H., Argo, E., Ayyad, Y., Bardayan, D., Bazin, D., Budner, T., Chen, A., Chipps, K., Davids, B., Dopfer, J., Friedman, M., Fynbo, H., Grzywacz, R., Jose, J., Liang, J., Mahajan, R., Pain, S., Pérez-Loureiro, D., Pollacco, E., Psaltis, A., Ravishankar, S., Rogers, A., Schaedig, L., Sun, L. J., Surbrook, J., Weghorn, L., and Wrede, C. Measuring the 15 O(α, γ) 19 Ne reaction in Type I X-ray bursts using the GADGET II TPC: Hardware. Retrieved from https://par.nsf.gov/biblio/10317808. EPJ Web of Conferences 260. Web. doi:10.1051/epjconf/202226011046.
Wheeler, Tyler, Adams, A., Allmond, J., Alvarez Pol, H., Argo, E., Ayyad, Y., Bardayan, D., Bazin, D., Budner, T., Chen, A., Chipps, K., Davids, B., Dopfer, J., Friedman, M., Fynbo, H., Grzywacz, R., Jose, J., Liang, J., Mahajan, R., Pain, S., Pérez-Loureiro, D., Pollacco, E., Psaltis, A., Ravishankar, S., Rogers, A., Schaedig, L., Sun, L. J., Surbrook, J., Weghorn, L., & Wrede, C. Measuring the 15 O(α, γ) 19 Ne reaction in Type I X-ray bursts using the GADGET II TPC: Hardware. EPJ Web of Conferences, 260 (). Retrieved from https://par.nsf.gov/biblio/10317808. https://doi.org/10.1051/epjconf/202226011046
Wheeler, Tyler, Adams, A., Allmond, J., Alvarez Pol, H., Argo, E., Ayyad, Y., Bardayan, D., Bazin, D., Budner, T., Chen, A., Chipps, K., Davids, B., Dopfer, J., Friedman, M., Fynbo, H., Grzywacz, R., Jose, J., Liang, J., Mahajan, R., Pain, S., Pérez-Loureiro, D., Pollacco, E., Psaltis, A., Ravishankar, S., Rogers, A., Schaedig, L., Sun, L. J., Surbrook, J., Weghorn, L., and Wrede, C.
"Measuring the 15 O(α, γ) 19 Ne reaction in Type I X-ray bursts using the GADGET II TPC: Hardware". EPJ Web of Conferences 260 (). Country unknown/Code not available. https://doi.org/10.1051/epjconf/202226011046.https://par.nsf.gov/biblio/10317808.
@article{osti_10317808,
place = {Country unknown/Code not available},
title = {Measuring the 15 O(α, γ) 19 Ne reaction in Type I X-ray bursts using the GADGET II TPC: Hardware},
url = {https://par.nsf.gov/biblio/10317808},
DOI = {10.1051/epjconf/202226011046},
abstractNote = {Sensitivity studies have shown that the 15 O(α, γ) 19 Ne reaction is the most important reaction rate uncertainty affecting the shape of light curves from Type I X-ray bursts. This reaction is dominated by the 4.03 MeV resonance in 19 Ne. Previous measurements by our group have shown that this state is populated in the decay sequence of 20 Mg. A single 20 Mg(βp α) 15 O event through the key 15 O(α, γ) 19 Ne resonance yields a characteristic signature: the emission of a proton and alpha particle. To achieve the granularity necessary for the identification of this signature, we have upgraded the Proton Detector of the Gaseous Detector with Germanium Tagging (GADGET) into a time projection chamber to form the GADGET II detection system. GADGET II has been fully constructed, and is entering the testing phase.},
journal = {EPJ Web of Conferences},
volume = {260},
author = {Wheeler, Tyler and Adams, A. and Allmond, J. and Alvarez Pol, H. and Argo, E. and Ayyad, Y. and Bardayan, D. and Bazin, D. and Budner, T. and Chen, A. and Chipps, K. and Davids, B. and Dopfer, J. and Friedman, M. and Fynbo, H. and Grzywacz, R. and Jose, J. and Liang, J. and Mahajan, R. and Pain, S. and Pérez-Loureiro, D. and Pollacco, E. and Psaltis, A. and Ravishankar, S. and Rogers, A. and Schaedig, L. and Sun, L. J. and Surbrook, J. and Weghorn, L. and Wrede, C.},
editor = {Liu, W. and Wang, Y. and Guo, B. and Tang, X. and Zeng, S.}
}
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