2015
DOI: 10.1007/jhep03(2015)104
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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

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Cited by 85 publications
(110 citation statements)
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References 108 publications
(289 reference statements)
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“…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%