2017
DOI: 10.1140/epjc/s10052-017-4627-x
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The one-loop contributions to c(t) electric dipole moment in the CP-violating BLMSSM

Abstract: In the CP-violating supersymmetric extension of the standard model with local gauged baryon and lepton symmetries (BLMSSM), there are new CP-violating sources which can give new contributions to the quark electric dipole moment (EDM). Considering the CP-violating phases, we analyze the EDMs of the quarks c and t. We take into account the contributions from the one-loop diagrams. The numerical results are analyzed with some assumptions on the relevant parameter space. The numerical results for the c and t EDMs … Show more

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Cited by 8 publications
(7 citation statements)
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“…Indirect bounds on charm (beauty) quark EDM are set from different experimental measurements and span over several orders of magnitude, i.e. charm (beauty) EDM < ∼ 10 −15 − 4.4 × 10 −17 e cm [11,12,13,14,15] ( < ∼ 2 × 10 −12 − 2 × 10 −17 e cm [13,14,15,16]), depending on different models and assumptions. As an example, an indirect bound on the charm quark EDM is derived from the experimental limit on the neutron EDM to be < ∼ 4.4 × 10 −17 e cm [11], and a charm quark EDM of comparable magnitude is possible in extensions of the SM [12].…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…Indirect bounds on charm (beauty) quark EDM are set from different experimental measurements and span over several orders of magnitude, i.e. charm (beauty) EDM < ∼ 10 −15 − 4.4 × 10 −17 e cm [11,12,13,14,15] ( < ∼ 2 × 10 −12 − 2 × 10 −17 e cm [13,14,15,16]), depending on different models and assumptions. As an example, an indirect bound on the charm quark EDM is derived from the experimental limit on the neutron EDM to be < ∼ 4.4 × 10 −17 e cm [11], and a charm quark EDM of comparable magnitude is possible in extensions of the SM [12].…”
Section: Introductionmentioning
confidence: 99%
“…charm (beauty) EDM < ∼ 10 −15 − 4.4 × 10 −17 e cm [11,12,13,14,15] ( < ∼ 2 × 10 −12 − 2 × 10 −17 e cm [13,14,15,16]), depending on different models and assumptions. As an example, an indirect bound on the charm quark EDM is derived from the experimental limit on the neutron EDM to be < ∼ 4.4 × 10 −17 e cm [11], and a charm quark EDM of comparable magnitude is possible in extensions of the SM [12]. For the beauty quark, indirect EDM limits < ∼ 2 × 10 −12 e cm [13] and < ∼ 1.22 × 10 −13 e cm [16] are derived, and a relatively large beauty quark EDM is possible in presence of new physics.…”
Section: Introductionmentioning
confidence: 99%
“…a 30% stronger bounds for M NP = 10 TeV. The new constraints for the charm and bottom quark EDMs are in tension with the predictions of different theories beyond the standard model [29][30][31][32] and will provide valuable input for future phenomenological analysis of NP models.…”
mentioning
confidence: 88%
“…[9], while the SM predicts a much smaller d n < 10 −31 e.cm [11]. There are similarly bounds on the c quark and t quark EDMs |d c | < 5.0 × 10 −17 e.cm and |d t | < 3.06 × 10 −15 e.cm [10].…”
Section: Introductionmentioning
confidence: 88%