Titlebook: Analysis of the Electric Dipole Moment in the R-parity Violating Supersymmetric Standard Model; Nodoka Yamanaka Book 2014 Springer Japan 2

PED

書目名稱Analysis of the Electric Dipole Moment in the R-parity Violating Supersymmetric Standard Model影響因子(影響力)




書目名稱Analysis of the Electric Dipole Moment in the R-parity Violating Supersymmetric Standard Model影響因子(影響力)學科排名




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書目名稱Analysis of the Electric Dipole Moment in the R-parity Violating Supersymmetric Standard Model網絡公開度學科排名




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書目名稱Analysis of the Electric Dipole Moment in the R-parity Violating Supersymmetric Standard Model讀者反饋




書目名稱Analysis of the Electric Dipole Moment in the R-parity Violating Supersymmetric Standard Model讀者反饋學科排名

露天歷史劇

強所

有危險

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R-parity Violation and Phenomenological Constraintstheir properties. We will then present briefly the bilinear R-parity violation, and finally list the phenomenological constraints on the trilinear R-parity violation given by particle physics experiments.

airborne

Atomic Level Calculationds and give their results. In the subsequent section, we will derive the contribution to the EDM of diamagnetic atoms using analytic formulae. We finally summarize the dependences of the EDMs of the relevant systems on P, CP-odd processes. Note that in this appendix the electric charge . is defined as ., the convention of Chap.?..

AIL

Constraints on Supersymmetric Models from Electric Dipole Momentsgent upper limits on them. In this chapter, we will see the constraints imposed on R-parity conserving supersymmetric models by the EDM experimental data via different microscopic P, CP-odd processes.

巫婆

Classification of RPV Couplings and RPV Dependence to EDM Observables on RPV bilinears derived from hadronic, nuclear and atomic level calculations, seen in detail in Part II. Roughly speaking, we will derive the linear coefficient of the EDM observable on the RPV bilinears. This is the zeroth step of our analysis.

SCORE

Analysis of the RPV Contribution to the P, CP-Odd 4-Fermion Interaction at the One-Loop Levelevel. This is because loop level diagrams can involve new RPV structures not encountered at the tree level. The analysis of the RPV contribution to the P, CP-odd 4-quark interaction at the one-loop level is also given, and prospective constraints from future experiments are shown.

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