Urca Processes in Stellar Degenerate Cores Dag Fahlin Strömberg

Urca Processes in Stellar Degenerate Cores Dag Fahlin Strömberg

Urca processes in stellar degenerate cores Dag Fahlin Strömberg Structure and Reactions for Nuclear Astrophysics 22-24 November 2017 IPHC, Strasbourg December 18, 2017 | IKP TUD | D. Fahlin Strömberg | 1 The fate of stars Heiko Möller, PhD Thesis (2017) December 18, 2017 | IKP TUD | D. Fahlin Strömberg | 2 Degenerate ONe cores 16 20 23 24 25 I Main content after carbon burning: O, Ne, Na, Mg and Mg. I Mainly supported by degeneracy pressure 1=3 I Electron Fermi energy EF ∼ ρ increases when the core contracts I Electron capture (EC) when EF is larger than the Q value I This corresponds to a specific density threshold ρ I Thresholds (Arnett, Supernovae and Nucleosynthesis): −3 Nucleus EF [MeV] 2Yeρ [g · cm ] 25Mg 3.833 1.17 × 109 23Na 4.374 1.67 × 109 24Mg 5.513 3.16 × 109 20Ne 7.026 6.20 × 109 16O 10.42 1.90 × 1010 December 18, 2017 | IKP TUD | D. Fahlin Strömberg | 3 Urca and double electron capture processes Heiko Möller, PhD Thesis (2017) December 18, 2017 | IKP TUD | D. Fahlin Strömberg | 4 Urca cooling in acreeting ONe white dwarfs I We study the evolution of acreeting ONe white dwarfs up to oxygen ignition I Conditions at ignition important for final outcome 20 24 I Heating from double electron capture: Ne and Mg 25 25 23 23 25 25 I Schwab et al. (2017): Urca pairs Mg & Na, Na & Ne and Na & Ne I This was also studied in Heiko Möller’s PhD thesis I Both used the MESA (Modules for Experiments in Stellar Astrophysics) stellar evolution code December 18, 2017 | IKP TUD | D. Fahlin Strömberg | 5 Urca cooling in acreeting ONe WD Schwab et. al, 2017. December 18, 2017 | IKP TUD | D. Fahlin Strömberg | 6 Unexplored: Effect of metallicity in ONe cores I Non-zero metallicity in the progenitor =) additional nuclei in ONe core I Piersant et al. (2017): I Studied effects of initial metallicity on SNe Ia (i.e. acreeting CO white dwarfs) I Included EC processes on the corresponding nuclei I Simulation: increased density and neutronization at thermal runaway I Thus: metallicity affects light curve of SNe Ia I But the effects of metallicity in ONe cores remain unexplored I This is what we are currently investigating, i.e. including EC procceses on additional nuclei from initial metallicity December 18, 2017 | IKP TUD | D. Fahlin Strömberg | 7 Nuclei considered in Piersanti et al. December 18, 2017 | IKP TUD | D. Fahlin Strömberg | 8 Additional nuclei for ONe cores I Nuclei above should also matter for ONe cores I But: Oxygen ignites at higher densities than carbon I Consequently: EC on larger set of nuclei prior to runaway I Rough selection: Order by abundance and choose most abundant December 18, 2017 | IKP TUD | D. Fahlin Strömberg | 9 Weak interaction rates I To include these effect we need accurate weak interaction rates I Traditional way: Tables of interaction rates, e.g. I Fuller, Fowler, and Newman (1980, 1982, 1985): sd & pf shells I Oda et al. (1994): sd shell I Langanke and Martínez-Pinedo (2001): pf shell I Suzuki et al. (2016): sd shell I Tables based on experimental data + shell model calculations I Problem: interpolation errors I Rates can quickly change several orders of magnitude I Newer tables (e.g. Suzuki et al.) have denser data points I But we still get issues at low temperatures (see Schwab et al. (2017)) December 18, 2017 | IKP TUD | D. Fahlin Strömberg | 10 Example: The Urca pair 31P and 31Si T = 7. 0 108 K × Denser table 4 Oda et al. 6 ¢ ] 1 − s [ 8 λ ¡ g o l 10 12 7.0 7.2 7.4 7.6 7.8 8.0 3 log ρYe [g cm− ] ¡ ¢ December 18, 2017 | IKP TUD | D. Fahlin Strömberg | 11 Alternative: Analytical determination I At these temperatures only low-lying excited states are relevant I Consequently the rates are typically determined by a few transitions I This means that we can compute the rates during the simulation I Phase space integrals can be approximated as an analytical expression (see Fuller, Fowler, and Newman (1985)) I This functionality has been implemented in the MESA stellar evolution code I We must identify relevant transitions December 18, 2017 | IKP TUD | D. Fahlin Strömberg | 12 Urca pair 25Mg and 25Na: Experimental data 1/2+ 3/2+ 4.0 5/2+ 25Na 3.0 3/2+ 2.0 5/2+ 7/2+ Energy (MeV) 1.0 3/2+ 1/2+ 0.0 5/2+ 25Mg December 18, 2017 | IKP TUD | D. Fahlin Strömberg | 13 Urca pair 25Mg and 25Na: Relevant transitions 1/2+ 3/2+ 4.0 5/2+ 25Na 3.0 3/2+ 2.0 5/2+ 7/2+ Energy (MeV) 1.0 3/2+ 1/2+ 0.0 5/2+ 25Mg December 18, 2017 | IKP TUD | D. Fahlin Strömberg | 14 25Mg and 25Na: What is the difference? log(T/K) = 8. 6 3 4 5 ¢ ] 1 6 − s [ λ ¡ g 7 o l 8 9 Experimental data Selected transitions 10 8.5 8.6 8.7 8.8 8.9 9.0 3 log ρYe [g cm− ] ¡ ¢ December 18, 2017 | IKP TUD | D. Fahlin Strömberg | 15 25Mg and 25Na: Are other transitions important? log(T/K) = 8. 6 3 4 5 ¢ ] 1 6 − s [ λ ¡ g 7 o l 8 9 Suzuki et al. Selected transitions 10 8.5 8.6 8.7 8.8 8.9 9.0 3 log ρYe [g cm− ] ¡ ¢ December 18, 2017 | IKP TUD | D. Fahlin Strömberg | 16 Beta decay of 56Mn 1+ 4.0 2+ 3+ 0.111 MeV 56Mn 3.0 4+ 2.0 Energy (MeV) 1.0 2+ 0.0 0+ 56Fe December 18, 2017 | IKP TUD | D. Fahlin Strömberg | 17 Beta decay of 56Mn log(T/K) = 8. 2 0 5 ¢ ] 1 − s [ 10 λ ¡ g o l 15 1 + 0 + → 2 + 2 + → 3 + 2 + → Total 20 8.0 8.2 8.4 8.6 8.8 9.0 3 log ρYe [g cm− ] ¡ ¢ December 18, 2017 | IKP TUD | D. Fahlin Strömberg | 18 Forbidden transition from 20Ne 20 I Martinez-Pinedo et al. (2014): forbidden transition important for EC on Ne December 18, 2017 | IKP TUD | D. Fahlin Strömberg | 19 Conclusions I Urca processes are important for the evolution of degenerate stellar cores I Rates are typically determined by few transitions — analytic determination of the rates I Accounting for initial composition of the star (metallicity) allows for additional EC processes that are currently being investigated 20 I Second forbidden transition from Ne still needs to be determined December 18, 2017 | IKP TUD | D. Fahlin Strömberg | 20 Appendix X (2J + 1) exp(−E =kt) λEC = P λEC P = i i if if if P (2J + 1) exp(−E =kt) if j j j P k + EC ln 2 EC 2 h f j k σ tk j i i λif = Bif φ (qif ) Bif (GT ) = gA K 2Ji + 1 Z 1 EC 2 φ (qif ) = wp(qif + w) F(Z, w)Se(w)dw wl December 18, 2017 | IKP TUD | D. Fahlin Strömberg | 21.

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