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$β$-decay Measurements Near the $N=40$ Island of Inversion to Quantify Cooling of Accreted Neutron Star Crusts

K. Hermansen, W. -J. Ong, H. Schatz, J. Browne, A. Chester, K. Childers, R. Jain, S. Liddick, S. Lyons, S. A. Miskovich, P. Möller, F. Montes, J. Owens-Fryar, A. Palmisano-Kyle, A. L. Richard, N. Rijal, M. Smith, D. Soltesz, A. Spyrou, S. K. Subedi, L. Wagner

Abstract

Understanding the thermal structure of the outer crust of accreting neutron stars is important to interpret astronomical X-ray observations. Ground-state to ground-state $β$-decay transitions of neutron-rich nuclei comprising the crust enable Urca neutrino cooling processes that affect this thermal structure. Here we constrain the ground-state to ground-state transition strengths for the decays of $^{57}$Sc, $^{57}$Ti, and $^{59}$Ti based on experimental data. The data were obtained by combining total absorption $γ$-spectroscopy data from the SuN detection system with $β$-delayed neutron emission data from the NERO detection system at Michigan State University's National Superconducting Cyclotron Laboratory. We find $\log ft=$5.8$^{+0.3}_{-0.2}$ and $\log ft=$5.34$^{+0.08}_{-0.24}$ for the decays of $^{57}$Ti and $^{59}$Ti, respectively, and find no evidence for ground-state feeding in the decay of $^{57}$Sc. The results indicate weaker transitions than predicted by theory and indicated by previous measurements, resulting in reduced efficiency of neutrino cooling in accreted neutron star crusts in systems that exhibit X-ray superbursts.

$β$-decay Measurements Near the $N=40$ Island of Inversion to Quantify Cooling of Accreted Neutron Star Crusts

Abstract

Understanding the thermal structure of the outer crust of accreting neutron stars is important to interpret astronomical X-ray observations. Ground-state to ground-state -decay transitions of neutron-rich nuclei comprising the crust enable Urca neutrino cooling processes that affect this thermal structure. Here we constrain the ground-state to ground-state transition strengths for the decays of Sc, Ti, and Ti based on experimental data. The data were obtained by combining total absorption -spectroscopy data from the SuN detection system with -delayed neutron emission data from the NERO detection system at Michigan State University's National Superconducting Cyclotron Laboratory. We find 5.8 and 5.34 for the decays of Ti and Ti, respectively, and find no evidence for ground-state feeding in the decay of Sc. The results indicate weaker transitions than predicted by theory and indicated by previous measurements, resulting in reduced efficiency of neutrino cooling in accreted neutron star crusts in systems that exhibit X-ray superbursts.
Paper Structure (11 sections, 12 figures, 5 tables)

This paper contains 11 sections, 12 figures, 5 tables.

Figures (12)

  • Figure 1: $P_{\rm n}$ values as functions of mass number for Sc isotopes (left) and V isotopes (right). Shown are the results from this work (red), results from previous work (black) crawfordDecayIsomericProperties2010bongDecay61VIts2020, and theoretical predictions from QRPA-fY (blue).
  • Figure 2: TAS (top), SS (bottom), and multiplicity (bottom inset) measured spectra (black) together with the corresponding template fits (red) for the decay of $^{57}$Ti. The black vertical line indicates a change in the energy axis scale. Blue triangles mark the neutron separation energy of the $^{57}$V daughter.
  • Figure 3: Discrete levels in $^{57}$V populated by the decay of $^{57}$Ti and associated $\gamma$-transitions used in this work. The newly identified transition is drawn in red. Dashed red lines indicate new tentative levels that have been inserted to improve the fits.
  • Figure 4: TAS (top), SS (bottom), and multiplicity (bottom inset) measured spectra (black) together with the corresponding template fits (red) for the decay of $^{57}$Sc. The vertical black line marks a change in energy axis scale. Blue triangles mark the neutron separation energy of the $^{57}$Ti daughter.
  • Figure 5: Discrete levels in $^{57}$Ti populated by the decay of $^{57}$Sc and associated $\gamma$-transitions used in this work. Newly identified levels and transitions are drawn in red. Dashed lines indicate tentative levels that have been inserted to improve the fits.
  • ...and 7 more figures