2015
DOI: 10.1007/jhep03(2015)104
|View full text |Cite|
|
Sign up to set email alerts
|

Nuclear electric dipole moments in chiral effective field theory

Abstract: We provide a consistent and complete calculation of the electric dipole moments of the deuteron, helion, and triton in the framework of chiral effective field theory. The CP-conserving and CP-violating interactions are treated on equal footing and we consider CP-violating one-, two-, and three-nucleon operators up to next-to-leading-order in the chiral power counting. In particular, we calculate for the first time EDM contributions induced by the CP-violating three-pion operator. We find that effects of CP-vio… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

11
97
1

Year Published

2015
2015
2022
2022

Publication Types

Select...
7
1

Relationship

4
4

Authors

Journals

citations
Cited by 81 publications
(109 citation statements)
references
References 108 publications
11
97
1
Order By: Relevance
“…Almost the same final results for M (θ) can be obtained by using recently calculated relations of g 0 and g 1 constants by using chiral perturbation theory [56] and lattice data for the strong part of the proton-neutron mass difference [57] which give updated value of gg 0 . Finally, we can express MQM in terms of the quark chromo-EDMd u andd d using the relations gḡ 1 = 4.·10 [58]:…”
Section: Nuclear Magnetic Quadrupole Momentsupporting
confidence: 56%
“…Almost the same final results for M (θ) can be obtained by using recently calculated relations of g 0 and g 1 constants by using chiral perturbation theory [56] and lattice data for the strong part of the proton-neutron mass difference [57] which give updated value of gg 0 . Finally, we can express MQM in terms of the quark chromo-EDMd u andd d using the relations gḡ 1 = 4.·10 [58]:…”
Section: Nuclear Magnetic Quadrupole Momentsupporting
confidence: 56%
“…The Weinberg operator is chiral invariant and therefore its contribution toḡ 0,1 is suppressed by m 2 π /Λ 2 χ where Λ χ ∼ 1 GeV [58,68]. Nevertheless, power counting indicates that nuclear EDMs can still significantly depend onḡ 0,1 induced by the Weinberg operator [68,72], but explicit calculations show that the largest contributions arise from the constituent nucleon EDMs [73,74]. We will therefore neglectḡ 0,1 from the Weinberg operator.…”
Section: Jhep02(2016)011mentioning
confidence: 99%
“…[72]. The 3 He EDM has been analyzed within the same framework [72,73] and depends onḡ 0 as well. In addition, it depends on CPV nucleon-nucleon interactions induced by the Weinberg operator.…”
Section: Jhep02(2016)011mentioning
confidence: 99%
“…A single EDM measurement would not be sufficient to identify the source of P and T violation and EDM measurements of several light nuclei are in general required to impose constraints on the sources of P and T violation within and beyond the SM [20][21][22][23][24][25]. This paper provides a detailed explanation of the formal but necessary aspects of the investigation of the EDMs of light nuclei, i.e.…”
Section: Introductionmentioning
confidence: 99%