Ab initio Description of Neutrinoless Double Beta Decay with the In-Medium Similarity Renormalization Group
ORAL
Abstract
Recently, there has been significant progress in ab initio calculations
of the nuclear matrix elements (NMEs) for neutrinoless double beta decay (NLDBD).
Methods like the In-Medium Similarity Renormalization Group (IMSRG) and
Coupled Cluster Theory have produced first results for candidate
nuclei based on interactions from chiral effective field theory [1,2,3], and
efforts are underway towards improved consistency and uncertainties.
In this context, Cirigliano et al. have pointed out the presence of a
leading-order counter term in the EFT-based NLDBD transition operator,
and proposed a protocol for determining its coupling [4]. We have
implemented this counter term and studied its impact in benchmark calculations
for light nuclei as well as the lightest realistic NLDBD candidate, 48Ca. Encouragingly,
we obtain a robust enhancement of the NMEs, although we stress
that fully consistent results are still pending.
[1] J. M. Yao et al., PRL 124, 232501
[2] A. Belley et al., PRL 126, 042502
[3] S. J. Novario et al., PRL 126, 182502
[4] V. Cirigliano et al., PRL 126, 172002
of the nuclear matrix elements (NMEs) for neutrinoless double beta decay (NLDBD).
Methods like the In-Medium Similarity Renormalization Group (IMSRG) and
Coupled Cluster Theory have produced first results for candidate
nuclei based on interactions from chiral effective field theory [1,2,3], and
efforts are underway towards improved consistency and uncertainties.
In this context, Cirigliano et al. have pointed out the presence of a
leading-order counter term in the EFT-based NLDBD transition operator,
and proposed a protocol for determining its coupling [4]. We have
implemented this counter term and studied its impact in benchmark calculations
for light nuclei as well as the lightest realistic NLDBD candidate, 48Ca. Encouragingly,
we obtain a robust enhancement of the NMEs, although we stress
that fully consistent results are still pending.
[1] J. M. Yao et al., PRL 124, 232501
[2] A. Belley et al., PRL 126, 042502
[3] S. J. Novario et al., PRL 126, 182502
[4] V. Cirigliano et al., PRL 126, 172002
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Publication: arXiv:2105.05415
Presenters
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Heiko Hergert
Michigan State University
Authors
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Heiko Hergert
Michigan State University
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Roland Wirth
Facility for Rare Isotope Beams, Michigan State University
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Jiangming Yao
Sun-Yat Sen University