2011
DOI: 10.1103/physrevc.84.044316
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Nonperturbative renormalization of the neutrinoless double-βoperator inp-shell nuclei

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Cited by 7 publications
(15 citation statements)
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References 28 publications
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“…Perhaps the most significant obstacle to a truly reliable result, however, is the implementation of induced three-body operators. Recent work [34,35] indicates that such operators are not negligible, and even here we have shown that three-body diagrams of the form in Fig. 4 are important.…”
Section: Discussion and Outlookmentioning
confidence: 99%
“…Perhaps the most significant obstacle to a truly reliable result, however, is the implementation of induced three-body operators. Recent work [34,35] indicates that such operators are not negligible, and even here we have shown that three-body diagrams of the form in Fig. 4 are important.…”
Section: Discussion and Outlookmentioning
confidence: 99%
“…[114], which for the first time tests the consistency of the SRG approach with a continuum observable, and the evaluation of neutrinoless doublebeta decay with SRG-evolved interactions in Ref. [115]. Adapting the RG technology developed for evolving and evaluating Hamiltonians to extend these and related studies to use fully consistent evolved operators is an important goal.…”
Section: Evolution Of Operators As An Rg Frontiermentioning
confidence: 99%
“…Some have been based on the ab-initio no-core shell model [12,13], via a valence-cluster expansion [14][15][16], and others on the in-medium similarity renormalization group [17]. In this Letter we use a third approach, the ab-initio coupled-cluster method [18][19][20][21][22][23], to construct effective shell-model interactions for use in open-shell and neutron-rich nuclei.…”
mentioning
confidence: 99%
“…-Here we report our CCEI results for ground and low-lying states in oxygen and carbon isotopes. We choose 16 O in oxygen and 14 C in carbon as the closedshell cores. We then project the one-and two-particleattached coupled-cluster wave functions onto the oneand two-particle model space states in the valence space -the d 5/2 , s 1/2 , d 3/2 shell -and proceed to use the resulting shell-model Hamiltonians in heavier isotopes.…”
mentioning
confidence: 99%