Ab initio calculations of nuclear structure corrections of super-allowed Fermi transitions
ORAL
Abstract
CKM unitarity is a sensitive probe of the Standard Model. The top row unitarity is dominated by the Vud matrix element which is most cleanly extracted from nuclear Fermi β decays. The most recent data-driven analyses of measurements suggest a 2σ−3σ discrepancy [1-2]. Several theoretical corrections are required to extract the Vud and, in fact, the current uncertainty in Vud extracted from Fermi transitions is dominated by theory. We perform ab initio calculations of nuclear structure corrections δNS and δC for the 10C→10B Fermi transition that suffer from substantial uncertainties. We apply the no-core shell model (NCSM) [3] to calculate the δNS with the nuclear Green’s function obtained using the continued fraction Lanczos algorithm [4] and NCSM with continuum (NCSMC) [5] to calculate the δC using the recently introduced NCSMC β-decay formalism [6]. We will report preliminary results for the δNS and report our progress towards the δC calculation. Our approach is also applicable to 14O→14N Fermi transition as well as to transitions in light sd shell nuclei.
[1] C.-Y. Seng, M. Gorchtein, H. H. Patel, M. J. Ramsey-Musolf, Phys. Rev. Lett. 121, 241804 (2018)
[2] M. Gorchtein, Phys. Rev. Lett. 123, 042503 (2019)
[3] B. R. Barrett, P. Navratil, J. P. Vary, Progress in Particle and Nuclear Physics 69, 131 (2013)
[4] M. A. Marchisio, N. Barnea, W. Leidemann, G. Orlandini, Few-Body Syst. 33, 259 (2003)
[5] S. Baroni, P. Navratil, and S. Quaglioni, Phys. Rev. Lett. 110, 022505 (2013); Phys. Rev. C 87, 034326 (2013)
[6] M. C. Atkinson, P. Navratil, G. Hupin, K. Kravvaris, S. Quaglioni, Phys. Rev. C 105, 054316 (2022)
[1] C.-Y. Seng, M. Gorchtein, H. H. Patel, M. J. Ramsey-Musolf, Phys. Rev. Lett. 121, 241804 (2018)
[2] M. Gorchtein, Phys. Rev. Lett. 123, 042503 (2019)
[3] B. R. Barrett, P. Navratil, J. P. Vary, Progress in Particle and Nuclear Physics 69, 131 (2013)
[4] M. A. Marchisio, N. Barnea, W. Leidemann, G. Orlandini, Few-Body Syst. 33, 259 (2003)
[5] S. Baroni, P. Navratil, and S. Quaglioni, Phys. Rev. Lett. 110, 022505 (2013); Phys. Rev. C 87, 034326 (2013)
[6] M. C. Atkinson, P. Navratil, G. Hupin, K. Kravvaris, S. Quaglioni, Phys. Rev. C 105, 054316 (2022)
*Supported by the NSERC Grant No. SAPIN-2022-00019 and by the U.S. Department of Energy, Office of Science, Office of Nuclear Physics, under Work Proposals No. SCW1158 and No. SCW0498. TRIUMF receives federal funding via a contribution agreement with the National Research Council of Canada. This work was prepared in part by LLNL under Contract No. DE-AC52-07NA27344. Computing support came from an INCITE Award on the Summit supercomputer of the Oak Ridge Leadership Computing Facility (OLCF) at ORNL, from the Digital Research Alliance of Canada, and from the LLNL institutional Computing Grand Challenge Program.
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Presenters
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Petr Navratil
- TRIUMF