Abstract

The ACME collaboration has recently announced a new constraint on the electron EDM, |de| < 1.1 × 10−29e cm, from measurements of the ThO molecule. This is a powerful constraint on CP-violating new physics: even new physics generating the EDM at two loops is constrained at the multi-TeV scale. We interpret the bound in the context of different scenarios for new physics: a general order-of-magnitude analysis for both the electron EDM and the CP-odd electron-nucleon coupling; 1-loop SUSY, probing sleptons above 10 TeV; 2-loop SUSY, probing multi-TeV charginos or stops; and finally, new physics that generates the EDM via the charm quark or top quark Yukawa couplings. In the last scenario, new physics generates a “QULE operator” left({q}_f{overline{sigma}}^{mu nu }{overline{u}}_fright)kern0.5em cdotp kern0.5em left(ell {overline{sigma}}_{mu nu}overline{e}right) , which in turn generates the EDM through RG evolution. If the QULE operator is generated at tree level, this corresponds to a previously studied leptoquark model. For the first time, we also classify scenarios in which the QULE operator is generated at one loop through a box diagram, which include (among others) SUSY and leptoquark models. The electron EDM bound is the leading constraint on a wide variety of theories of CP-violating new physics interacting with the Higgs boson or the top quark. We argue that any future nonzero measurement of an electron EDM will provide a strong motivation for constructing new colliders at the highest feasible energies.

Highlights

  • The ACME collaboration has used ThO molecules to constrain the electron electric dipole moment (EDM) to be [1]|de| < 1.1 × 10−29 e cm. (1.1)This is about an order of magnitude improvement on the previous bound from ACME [2] and from studies of HfF+ at JILA [3]

  • We interpret the bound in the context of different scenarios for new physics: a general order-of-magnitude analysis for both the electron EDM and the CP-odd electron-nucleon coupling; 1-loop SUSY, probing sleptons above 10 TeV; 2-loop SUSY, probing multi-TeV charginos or stops; and new physics that generates the EDM via the charm quark or top quark Yukawa couplings

  • In the Standard Model, this symmetry is violated by a handful of parameters: the CKM phase, which generates an electron EDM only at four loops with |de| ∼ 10−44 e cm and a CP-odd electron-nucleon interaction that can mimic an EDM of size |de| ∼ 10−38 e cm [4]; the strong phase θ, which generates an electron EDM |de| 10−37 e cm [7, 8]; and phases associated with the lepton sector, which give contributions at two loops suppressed by neutrino masses [9] with an expectation that |de| 10−43 e cm or, in the presence of severe fine-tuning, at most |de| 10−33 e cm [10]

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Summary

Introduction

The ACME collaboration has used ThO molecules to constrain the electron electric dipole moment (EDM) to be [1]. (If the up quark is the leading coupling, the CP-odd electron-nucleon coupling plays a more important role in the ThO measurement than the electron EDM itself.) The QULE operator could be induced by scalar leptoquark exchange at tree level, as previously discussed in [41,42,43]. It could arise from a box diagram, a case that we discuss for the first time. We argue that in the latter case, these new particles would lead to a very concrete form of the hierarchy problem, motivating the construction of new colliders even if the particles directly contributing to the EDM are out of reach

The electron EDM
An alternative: the CP-odd electron-nucleon coupling
77 MeV mt
The EDM constraint on one-loop SUSY
The EDM constraint on two-loop split SUSY
The EDM constraint on natural SUSY
The RGE of the electron EDM
One loop EDM from tree level QULE
Two loop EDM from one loop QULE
Conclusions
Null results and new physics: spontaneously broken CP?
An EDM would reify the hierarchy problem
Findings
A Classification of QULE box diagrams
Full Text
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