Origin of configuration instabilities in the DFT-NCCI calculation

Investigate the origin of the instabilities produced by the excluded configurations C_5^{\rm B}, C_{11}^{\rm B}, and C_{14}^{\rm B} in the DFT-NCCI calculation of the lowest I=0, T=1 state in ^{10}B and the associated isospin-symmetry-breaking correction to the superallowed ^{10}C\rightarrow^{10}B beta decay.

Background

The DFT-NCCI calculations for {10}B exhibit instabilities associated with three configurations, C_5{\rm B}, C_{11}{\rm B}, and C_{14}{\rm B}. The most pronounced instability occurs for C_5{\rm B}, which produces an anomalously low excitation energy for the projected T=0 state and substantially affects the calculated isospin-symmetry-breaking correction, despite having only a minor effect on the energy of the lowest I=0, T=1 state.

Because these configurations were excluded from the final {10}B configuration space, the resulting configuration space is asymmetric and may introduce an unphysical isospin-breaking contribution. The authors explicitly identify the physical or computational origin of these instabilities as unresolved, making their clarification necessary for a more reliable assessment of the configuration-interaction contribution to the decay correction.

References

The origin of these instabilities is not yet understood and requires further investigation

Influence of configuration-interaction on isospin impurities and isospin symmetry breaking corrections to superallowed $0^+\rightarrow 0^+$ beta decays  (2609.03545 - Wysocki et al., 3 Sep 2026) in Section 3.2, subsection “The results for isospin-symmetry breaking correction”